a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models Logo
NPSMEFTd6 Class Reference

A model class for new physics in the form of the dimension-six effective Lagrangian. More...

#include <NPSMEFTd6.h>

+ Inheritance diagram for NPSMEFTd6:

Detailed Description

A model class for new physics in the form of the dimension-six effective Lagrangian.

Author
HEPfit Collaboration

This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPSMEFTd6_LFU_QFU" to assume lepton and quark flavour universality)

In this class we consider the dimension-six effective Lagrangian

\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]

The implementation is written in the basis of [132]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters contains 4 redundancies, given by the coefficients \(C_{2B,2W,DHB,DHW,DB,DW} \), which correspond to operators not included in the basis of [132]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.

Initialization

After creating an instance of the current class with the constructor NPSMEFTd6(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().

Model parameters

The model parameters of NPSMEFTd6 are summarized below:

Label LaTeX symbol Description
CG \(C_{G} \) The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW \(C_{W} \) The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
C2B \(C_{2B} \) The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.)
C2W \(C_{2W} \) The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.)
C2BS \(C_{2B}^{SILH} \) The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.)
C2WS \(C_{2W}^{SILH} \) The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.)
CHG \(C_{HG} \) The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW \(C_{HW} \) The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB \(C_{HB} \) The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CDHB \(C_{DHB} \) The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\).
CDHW \(C_{DHW}\) The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\).
CDB \(C_{DB} \) The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.)
CDW \(C_{DW}\) The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.)
CWB \(C_{WB} \) The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD \(C_{HD}\) The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CT \(C_{T}\) The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\).
CHbox \(C_{H\Box}\) The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH \(C_{H}\) The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1_kk, CHL1_klr, CHL1_kli \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\).
CHL3_kk, CHL3_klr, CHL3_kli \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)\), for \(i,j=1,2,3\).
CHe_kk, CHe_klr, CHe_kli \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\).
CHQ1_kk, CHQ1_klr, CHQ1_kli \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\).
CHQ3_kk, CHQ3_klr, CHQ3_kli \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)\), for \(i,j=1,2,3\).
CHu_kk, CHu_klr, CHu_kli \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\).
CHd_kk, CHd_klr, CHd_kli \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CHud_klr, CHud_kli \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\).
CeH_klr, CeH_kli \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\).
CuH_klr, CuH_kli \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\).
CdH_klr, CdH_kli \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\).
CuG_klr, CuG_kli \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CuW_klr, CuW_kli \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CuB_klr, CuB_kli \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\).
CdG_klr, CdG_kli \(\mbox{Re}\big[(C_{dG})_{kl}\big], \mbox{Im}\big[(C_{dG})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\), for \(i,j=1,2,3\).
CdW_klr, CdW_kli \(\mbox{Re}\big[(C_{dW})_{kl}\big], \mbox{Im}\big[(C_{dW})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CdB_klr, CdB_kli \(\mbox{Re}\big[(C_{dB})_{kl}\big], \mbox{Im}\big[(C_{dB})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\).
CeW_klr, CeW_kli \(\mbox{Re}\big[(C_{eW})_{kl}\big], \mbox{Im}\big[(C_{eW})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\).
CeB_klr, CeB_kli \(\mbox{Re}\big[(C_{eB})_{kl}\big], \mbox{Im}\big[(C_{eB})_{kl}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\).
CLL_1221, CLL_2112 \((C_{LL})_{1221,2112}\) The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
CLQ1 \(C_{LQ}^{(1)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3 \(C_{LQ}^{(3)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\).
Cee \(C_{EE}\) The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu \(C_{EU}\) The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced \(C_{ED}\) The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe \(C_{LE}\) The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu \(C_{LU}\) The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd \(C_{LD}\) The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe \(C_{QE}\) The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Lambda_NP \(\Lambda \) The new physics scale.
BrHinv Br \((H\to invisible)\) The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.)
BrHexo Br \((H\to exotic)\) The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.)
dg1Z \(\delta g_{1Z}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
dKappaga \(\delta \kappa_{\gamma}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
lambZ \(\lambda_{Z}\) Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.)
eXint \(\varepsilon_{X}^{int}\) The relative intrinsic theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.)
eXpar \(\varepsilon_{X}^{par}\) The relative parametric theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.)
eVBFE_i \(\varepsilon_{VBF}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\)
eWHE_i \(\varepsilon_{WH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\)
eZHE_i \(\varepsilon_{ZH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\)
ettHE_i \(\varepsilon_{ttH}^i(E)\) The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\)

Where the hermitian derivatives are defined as

\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]

and

\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\sigma^a D_\mu - \overset{\leftarrow}{D}_\mu \sigma^a)H. \]

Alternatively, when using the model name "NPSMEFTd6_LFU_QFU", where lepton and quark flavour universality are assumed (except for \((C_{fH})_{ij},~f=e,u,d\) which are assumed to be diagonal only), the parameters to be used as inputs for the dimension six coefficients are the following:

Label LaTeX symbol Description
CG \(C_{G} \) The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\).
CW \(C_{W} \) The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\).
C2B \(C_{2B} \) The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.)
C2W \(C_{2W} \) The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.)
C2BS \(C_{2B}^{SILH} \) The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.)
C2WS \(C_{2W}^{SILH} \) The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.)
CHG \(C_{HG} \) The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\).
CHW \(C_{HW} \) The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\).
CHB \(C_{HB} \) The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\).
CDHB \(C_{DHB} \) The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\).
CDHW \(C_{DHW}\) The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\).
CDB \(C_{DB} \) The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.)
CDW \(C_{DW}\) The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.)
CWB \(C_{WB} \) The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\).
CHD \(C_{HD}\) The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\).
CT \(C_{T}\) The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\).
CHbox \(C_{H\Box}\) The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\).
CH \(C_{H}\) The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\).
CHL1 \( (C_{HL}^{(1)})_{ii} \) The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal).
CHL3 \( (C_{HL}^{(3)})_{ii} \) The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^i\big)\) (flavor universal).
CHe \( (C_{He})_{ii} \) The coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal).
CHQ1 \( (C_{HQ}^{(1)})_{ii} \) The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal).
CHQ3 \( (C_{HQ}^{(3)})_{ii}\) The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^i\big)\) (flavor universal).
CHu \( (C_{Hu})_{ii} \) The coefficient of the operator \(({\cal O}_{Hu})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal).
CHd \( (C_{Hd})_{ii} \) The coefficient of the operator \(({\cal O}_{Hd})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CHud_r, CHud_i \(\mbox{Re}\big[(C_{Hud})_{ii}\big], \mbox{Im}\big[(C_{Hud})_{ii}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal).
CeH_jjr, CeH_jji \(\mbox{Re}\big[(C_{eH})_{jj}\big], \mbox{Im}\big[(C_{eH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{jj} =\big(H^\dagger H\big) \big(\overline{L^j}\,H E^j\big)\) (flavor universal).
CuH_jjr, CuH_jji \(\mbox{Re}\big[(C_{uH})_{jj}\big], \mbox{Im}\big[(C_{uH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,\widetilde{H} U^j\big)\) (flavor universal).
CdH_jjr, CdH_jji \(\mbox{Re}\big[(C_{dH})_{jj}\big], \mbox{Im}\big[(C_{dH})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,H D^j\big)\) (flavor universal).
CuG_jjr, CuG_jji \(\mbox{Re}\big[(C_{uG})_{jj}\big], \mbox{Im}\big[(C_{uG})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\) (flavor universal).
CuW_jjr, CuW_jji \(\mbox{Re}\big[(C_{uW})_{jj}\big], \mbox{Im}\big[(C_{uW})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\) (flavor universal).
CuB_jjr, CuB_jji \(\mbox{Re}\big[(C_{uB})_{jj}\big], \mbox{Im}\big[(C_{uB})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\) (flavor universal).
CdG_jjr, CdG_jji \(\mbox{Re}\big[(C_{dG})_{jj}\big], \mbox{Im}\big[(C_{dG})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\) (flavor universal).
CdW_jjr, CdW_jji \(\mbox{Re}\big[(C_{dW})_{jj}\big], \mbox{Im}\big[(C_{dW})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\) (flavor universal).
CdB_jjr, CdB_jji \(\mbox{Re}\big[(C_{dB})_{jj}\big], \mbox{Im}\big[(C_{dB})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\) (flavor universal).
CeW_jjr, CeW_jji \(\mbox{Re}\big[(C_{eW})_{jj}\big], \mbox{Im}\big[(C_{eW})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{jj} =\big(\overline{L^j}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\) (flavor universal).
CeB_jjr, CeB_jji \(\mbox{Re}\big[(C_{eB})_{jj}\big], \mbox{Im}\big[(C_{eB})_{jj}\big] \) The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{jj} =\big(\overline{L^j}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\) (flavor universal).
CLL \((C_{LL})_{1221,2112}\) The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\).
CLQ1 \(C_{LQ}^{(1)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\).
CLQ3 \(C_{LQ}^{(3)}\) The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\).
Cee \(C_{EE}\) The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Ceu \(C_{EU}\) The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
Ced \(C_{ED}\) The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CLe \(C_{LE}\) The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
CLu \(C_{LU}\) The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\).
CLd \(C_{LD}\) The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\).
CQe \(C_{QE}\) The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\).
Lambda_NP \(\Lambda \) The new physics scale.
BrHinv Br \((H\to invisible)\) The branching ratio of invisible Higgs decays. (Not part of the EFT. Only for tests.)
BrHexo Br \((H\to exotic)\) The branching ratio of exotic Higgs decays. (Not part of the EFT. Only for tests.)

(The parameters associated to the theoretical uncertainties: \(\varepsilon_{X}^{int}\), \(\varepsilon_{X}^{par}\) and \(\varepsilon_{X}^i(E)\), are the same for both "NPSMEFTd6" and "NPSMEFTd6_LFU_QFU".)

Model flags

The Flags of NPSMEFTd6 are summarized below:

Label Value Description
QuadraticTerms TRUE / FALSE This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized.
RotateCHWCHB TRUE / FALSE This flag is set to TRUE if using {sW2*CHW+cW2*CHB, -cW2*CHW+sW2*CHB} instead of {CHW, CHB} as floating parameters. The default value is FALSE.
PartialQFU TRUE / FALSE This flag is set to TRUE if using CHQ1_11=CHQ1_22, CHQ3_11=CHQ3_22, CHU_11=CHU_22, CHD_11=CHD_22, CHud_11=CHud_22.} Only applies in the Non QFU case. In that case only the (1,1) component is taken into account. The default value is FALSE.
FlavU3OfX TRUE / FALSE This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\). If TRUE, the operator coefficient is proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficient of third family. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE.
FlagUnivOfX TRUE / FALSE This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\) plus they are the same for all fermions. If TRUE, all the operator coefficients are proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficients of third family for \(O_{uH}\) and \(O_{uV}\), respectively. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE.
HiggsSM TRUE / FALSE This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE.
LoopHd6 TRUE / FALSE This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE.
LoopH3d6Quad TRUE / FALSE

This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE.

Important member functions

See the base classes of the current class.

Definition at line 885 of file NPSMEFTd6.h.

Public Member Functions

gslpp::complex AH_f (const double tau) const
 Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex AH_W (const double tau) const
 W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More...
 
gslpp::complex AHZga_f (const double tau, const double lambda) const
 Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex AHZga_W (const double tau, const double lambda) const
 W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual double aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
 
virtual double AuxObs_NP1 () const
 Auxiliary observable AuxObs_NP1 (See code for details.) More...
 
virtual double AuxObs_NP10 () const
 Auxiliary observable AuxObs_NP10 (See code for details.) More...
 
virtual double AuxObs_NP11 () const
 Auxiliary observable AuxObs_NP11 (See code for details.) More...
 
virtual double AuxObs_NP12 () const
 Auxiliary observable AuxObs_NP12 (See code for details.) More...
 
virtual double AuxObs_NP13 () const
 Auxiliary observable AuxObs_NP13. More...
 
virtual double AuxObs_NP14 () const
 Auxiliary observable AuxObs_NP14. More...
 
virtual double AuxObs_NP15 () const
 Auxiliary observable AuxObs_NP15. More...
 
virtual double AuxObs_NP16 () const
 Auxiliary observable AuxObs_NP16. More...
 
virtual double AuxObs_NP17 () const
 Auxiliary observable AuxObs_NP17. More...
 
virtual double AuxObs_NP18 () const
 Auxiliary observable AuxObs_NP18. More...
 
virtual double AuxObs_NP19 () const
 Auxiliary observable AuxObs_NP19. More...
 
virtual double AuxObs_NP2 () const
 Auxiliary observable AuxObs_NP2 (See code for details.) More...
 
virtual double AuxObs_NP20 () const
 Auxiliary observable AuxObs_NP20. More...
 
virtual double AuxObs_NP3 () const
 Auxiliary observable AuxObs_NP3 (See code for details.) More...
 
virtual double AuxObs_NP4 () const
 Auxiliary observable AuxObs_NP4 (See code for details.) More...
 
virtual double AuxObs_NP5 () const
 Auxiliary observable AuxObs_NP5 (See code for details.) More...
 
virtual double AuxObs_NP6 () const
 Auxiliary observable AuxObs_NP6 (See code for details.) More...
 
virtual double AuxObs_NP7 () const
 Auxiliary observable AuxObs_NP7 (See code for details.) More...
 
virtual double AuxObs_NP8 () const
 Auxiliary observable AuxObs_NP8 (See code for details.) More...
 
virtual double AuxObs_NP9 () const
 Auxiliary observable AuxObs_NP9 (See code for details.) More...
 
virtual double bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
 
virtual double Br_H_exo () const
 The branching ratio of the of the Higgs into exotic particles. More...
 
virtual double Br_H_inv () const
 The branching ratio of the of the Higgs into invisible particles. More...
 
virtual double Br_H_inv_NP () const
 The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More...
 
virtual double BrHbbRatio () const
 The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More...
 
virtual double BrHccRatio () const
 The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More...
 
virtual double BrHgagaRatio () const
 The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHggRatio () const
 The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More...
 
virtual double BrHmumuRatio () const
 The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More...
 
virtual double BrHtautauRatio () const
 The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More...
 
virtual double BrHtoinvRatio () const
 The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More...
 
virtual double BrHvisRatio () const
 The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More...
 
virtual double BrHWffRatio () const
 The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHWjjRatio () const
 The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More...
 
virtual double BrHWlvRatio () const
 The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHWW2l2vRatio () const
 The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHWW4fRatio () const
 The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHWW4jRatio () const
 The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
virtual double BrHWWRatio () const
 The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More...
 
virtual double BrHZddRatio () const
 The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual double BrHZffRatio () const
 The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHZgaeeRatio () const
 The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZgallRatio () const
 The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZgamumuRatio () const
 The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZgaRatio () const
 The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
virtual double BrHZllRatio () const
 The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZuuRatio () const
 The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual double BrHZvvRatio () const
 The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ2e2muRatio () const
 The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4dRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4eRatio () const
 The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4fRatio () const
 The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual double BrHZZ4lRatio () const
 The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4muRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4uRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual double BrHZZ4vRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
virtual double BrHZZRatio () const
 The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual double cgaga_HB () const
 The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cgg_HB () const
 The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cggEff_HB () const
 The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual bool CheckParameters (const std::map< std::string, double > &DPars)
 A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization. More...
 
double CLL_bottom () const
 
double CLL_charm () const
 
double CLL_down () const
 
double CLL_mu () const
 
double CLL_strange () const
 
double CLL_tau () const
 
double CLL_up () const
 
double CLR_bottom () const
 
double CLR_charm () const
 
double CLR_down () const
 
double CLR_mu () const
 
double CLR_strange () const
 
double CLR_tau () const
 
double CLR_up () const
 
virtual double computeGammaTotalRatio () const
 The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More...
 
double CRL_bottom () const
 
double CRL_charm () const
 
double CRL_down () const
 
double CRL_mu () const
 
double CRL_strange () const
 
double CRL_tau () const
 
double CRL_up () const
 
double CRR_bottom () const
 
double CRR_charm () const
 
double CRR_down () const
 
double CRR_mu () const
 
double CRR_strange () const
 
double CRR_tau () const
 
double CRR_up () const
 
virtual double cZBox_HB () const
 The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cZga_HB () const
 The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double cZZ_HB () const
 The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaa0 () const
 The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaa02 () const
 The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaMZ () const
 The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaMZ2 () const
 The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaSMZ () const
 The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaaSMZ2 () const
 The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltacZ_HB () const
 The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaG1_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
 
virtual double deltaG1_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
 
virtual double deltaG1_hZARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual double deltaG1_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
 
virtual double deltag1ZNP () const
 The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More...
 
virtual double deltag1ZNPEff () const
 The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
 
virtual double deltaG2_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
 
virtual double deltaG2_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
 
virtual double deltaG2_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
 
virtual double deltaG3_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
 
virtual double deltaG3_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
 
double deltag3G () const
 The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More...
 
gslpp::complex deltaG_Aff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Gff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaG_hAA () const
 The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
 
virtual double deltaG_hAARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
gslpp::complex deltaG_hAff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual gslpp::complex deltaG_hff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
 
gslpp::complex deltaG_hGff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaG_hgg () const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
 
virtual double deltaG_hggRatio () const
 The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual double deltaG_hhhRatio () const
 The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
 
gslpp::complex deltaG_hZff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Zff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More...
 
virtual double deltaGA_f (const Particle p) const
 New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual double deltaGamma_W () const
 The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More...
 
virtual double deltaGamma_Wff (const Particle fi, const Particle fj) const
 The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
double deltaGammaHbbRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHbbRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHccRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHccRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHgagaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHgagaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHggRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
double deltaGammaHggRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHtautauRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHtautauRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWjjRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWjjRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWlvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWlvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW2l2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW2l2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4jRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWW4jRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWWRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHWWRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZddRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZddRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZeeRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZeeRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZgaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZgaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZllRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZllRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZuuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZuuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZvvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZvvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ2e2muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ2e2muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4eRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4eRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4lRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4lRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZ4vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
double deltaGammaHZZRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
virtual double deltaGammaTotalRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
virtual double deltaGammaTotalRatio1noError () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More...
 
virtual double deltaGammaTotalRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More...
 
virtual double DeltaGF () const
 New physics contribution to the Fermi constant. More...
 
double deltaGL_f (const Particle p) const
 New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
 
virtual gslpp::complex deltaGL_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
gslpp::complex deltaGL_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
double deltaGL_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More...
 
virtual double deltaGmu () const
 The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaGmu2 () const
 The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
double deltaGR_f (const Particle p) const
 New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
 
virtual gslpp::complex deltaGR_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
gslpp::complex deltaGR_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
double deltaGR_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More...
 
virtual double deltaGV_f (const Particle p) const
 New physics contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual double deltaGwd6 () const
 The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More...
 
virtual double deltaGwd62 () const
 The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More...
 
virtual double deltaGzd6 () const
 The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More...
 
virtual double deltaGzd62 () const
 The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More...
 
virtual double deltaKgammaNP () const
 The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More...
 
virtual double deltaKgammaNPEff () const
 The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
 
virtual double deltamb () const
 The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamb2 () const
 The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamc () const
 The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamc2 () const
 The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMh () const
 The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMh2 () const
 The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamt () const
 The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamt2 () const
 The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamtau () const
 The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltamtau2 () const
 The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMwd6 () const
 The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More...
 
virtual double deltaMwd62 () const
 The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More...
 
virtual double deltaMz () const
 The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltaMz2 () const
 The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual double deltayb_HB () const
 The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltayc_HB () const
 The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaymu_HB () const
 The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltayt_HB () const
 The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double deltaytau_HB () const
 The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double dxseeWWdcos (const double sqrt_s, const double cos) const
 The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More...
 
virtual double dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const
 The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More...
 
gslpp::complex f_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex g_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
double GammaHbbRatio () const
 The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More...
 
double GammaHccRatio () const
 The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More...
 
double GammaHgagaRatio () const
 The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
double GammaHggRatio () const
 The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More...
 
double GammaHmumuRatio () const
 The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More...
 
double GammaHtautauRatio () const
 The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More...
 
double GammaHWffRatio () const
 The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHWjjRatio () const
 The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More...
 
double GammaHWlvRatio () const
 The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHWW2l2vRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHWW4fRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHWW4jRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
double GammaHWWRatio () const
 The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More...
 
double GammaHZddRatio () const
 The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
double GammaHZeeRatio () const
 The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More...
 
double GammaHZffRatio () const
 The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHZgaRatio () const
 The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
double GammaHZllRatio () const
 The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHZmumuRatio () const
 The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZuuRatio () const
 The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
double GammaHZvvRatio () const
 The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ2e2muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4dRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4eRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4fRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
double GammaHZZ4lRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
double GammaHZZ4uRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
double GammaHZZ4vRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
double GammaHZZRatio () const
 The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual double GammaW () const
 The total width of the \(W\) boson, \(\Gamma_W\). More...
 
virtual double GammaW (const Particle fi, const Particle fj) const
 A partial decay width of the \(W\) boson decay into a SM fermion pair. More...
 
double getCed_1123 () const
 Return NP coeff Ced_1123. More...
 
double getCed_2223 () const
 Return NP coeff Ced_2223. More...
 
double getCeu_1133 () const
 Return NP coeff Ceu_1133. More...
 
double getCeu_2233 () const
 Return NP coeff Ceu_2233. More...
 
double getCHe_11 () const
 Return NP coeff CHe_11. More...
 
double getCHe_22 () const
 Return NP coeff CHe_22. More...
 
double getCHL1_11 () const
 Return NP coeff CHL1_11. More...
 
double getCHL1_22 () const
 Return NP coeff CHL1_22. More...
 
double getCHL3_11 () const
 Return NP coeff CHL3_11. More...
 
double getCHL3_22 () const
 Return NP coeff CHL3_22. More...
 
double getCLd_1123 () const
 Return NP coeff CLd_1123. More...
 
double getCLd_2223 () const
 Return NP coeff CLd_2223. More...
 
double getCLedQ_11 () const
 Return NP coeff CLedq_11. More...
 
double getCLedQ_22 () const
 Return NP coeff CLedq_22. More...
 
double getCLQ1_1123 () const
 Return NP coeff CLQ1_1123. More...
 
double getCLQ1_2223 () const
 Return NP coeff CLQ1_2223. More...
 
double getCLQ3_1123 () const
 Return NP coeff CLQ3_1123. More...
 
double getCLQ3_2223 () const
 Return NP coeff CLQ3_2223. More...
 
double getCLu_1133 () const
 Return NP coeff CLu_1133. More...
 
double getCLu_2233 () const
 Return NP coeff CLu_2233. More...
 
double getCpLedQ_11 () const
 Return NP coeff CpLedq_11. More...
 
double getCpLedQ_22 () const
 Return NP coeff CpLedq_22. More...
 
double getCQe_2311 () const
 Return NP coeff CQe_2322. More...
 
double getCQe_2322 () const
 Return NP coeff CQe_2322. More...
 
double getLambda_NP () const
 Return Lambda_NP. More...
 
virtual NPSMEFTd6MatchinggetMatching () const
 A method to get the Matching object for this model. More...
 
gslpp::complex I_triangle_1 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex I_triangle_2 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual double kappaAeff () const
 The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More...
 
virtual double kappabeff () const
 The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More...
 
virtual double kappaceff () const
 The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More...
 
virtual double kappaGeff () const
 The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More...
 
virtual double kappamueff () const
 The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More...
 
virtual double kappataueff () const
 The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More...
 
virtual double kappaWeff () const
 The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More...
 
virtual double kappaZAeff () const
 The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More...
 
virtual double kappaZeff () const
 The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More...
 
virtual double lambdaZNP () const
 The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More...
 
virtual double lambz_HB () const
 The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual double mueeHvv (const double sqrt_s) const
 The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeHvvPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueettH (const double sqrt_s) const
 The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueettHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWBF (const double sqrt_s) const
 The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWW (const double sqrt_s) const
 The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeWWPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZBF (const double sqrt_s) const
 The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZH (const double sqrt_s) const
 The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZllH (const double sqrt_s) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZqqH (const double sqrt_s) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muepWBF (const double sqrt_s) const
 The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double muepZBF (const double sqrt_s) const
 The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual double muggH (const double sqrt_s) const
 The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual double muggHbb (const double sqrt_s) const
 The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muggHgaga (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muggHH (const double sqrt_s) const
 The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More...
 
virtual double muggHmumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muggHpttH (const double sqrt_s) const
 The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muggHtautau (const double sqrt_s) const
 The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muggHWW (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muggHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muggHZga (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muggHZZ (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muggHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double mummH (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More...
 
virtual double mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const
 The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More...
 
virtual double mutHq (const double sqrt_s) const
 The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muTHUggHbb (const double sqrt_s) const
 The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHgaga (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUggHmumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHtautau (const double sqrt_s) const
 The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHWW (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZga (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZgamumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZZ (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUggHZZ4mu (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHbb (const double sqrt_s) const
 The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHgaga (const double sqrt_s) const
 The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUttHmumu (const double sqrt_s) const
 The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHtautau (const double sqrt_s) const
 The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHWW (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHZga (const double sqrt_s) const
 The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHZZ (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUttHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFBRinv (const double sqrt_s) const
 The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
 
virtual double muTHUVBFHbb (const double sqrt_s) const
 The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHgaga (const double sqrt_s) const
 The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHinv (const double sqrt_s) const
 The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHmumu (const double sqrt_s) const
 The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHtautau (const double sqrt_s) const
 The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHWW (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHZga (const double sqrt_s) const
 The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHZZ (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVBFHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHbb (const double sqrt_s) const
 The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHBRinv (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
 
virtual double muTHUVHgaga (const double sqrt_s) const
 The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUVHinv (const double sqrt_s) const
 The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
 
virtual double muTHUVHmumu (const double sqrt_s) const
 The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHtautau (const double sqrt_s) const
 The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHWW (const double sqrt_s) const
 The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHZga (const double sqrt_s) const
 The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHZZ (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUVHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHbb (const double sqrt_s) const
 The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHgaga (const double sqrt_s) const
 The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUWHmumu (const double sqrt_s) const
 The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHtautau (const double sqrt_s) const
 The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHWW (const double sqrt_s) const
 The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHZga (const double sqrt_s) const
 The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHZZ (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUWHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHbb (const double sqrt_s) const
 The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHgaga (const double sqrt_s) const
 The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muTHUZHmumu (const double sqrt_s) const
 The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHtautau (const double sqrt_s) const
 The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHWW (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHZga (const double sqrt_s) const
 The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHZZ (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muTHUZHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muttH (const double sqrt_s) const
 The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muttHbb (const double sqrt_s) const
 The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muttHgaga (const double sqrt_s) const
 The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muttHmumu (const double sqrt_s) const
 The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muttHtautau (const double sqrt_s) const
 The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muttHWW (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muttHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muttHZbbboost (const double sqrt_s) const
 The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More...
 
virtual double muttHZga (const double sqrt_s) const
 The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muttHZZ (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muttHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muVBF (const double sqrt_s) const
 The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual double muVBFgamma (const double sqrt_s) const
 The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More...
 
virtual double muVBFHbb (const double sqrt_s) const
 The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muVBFHgaga (const double sqrt_s) const
 The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muVBFHmumu (const double sqrt_s) const
 The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muVBFHtautau (const double sqrt_s) const
 The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muVBFHWW (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muVBFHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZga (const double sqrt_s) const
 The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZZ (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muVBFHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muVBFpVH (const double sqrt_s) const
 The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muVH (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muVHbb (const double sqrt_s) const
 The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muVHgaga (const double sqrt_s) const
 The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muVHmumu (const double sqrt_s) const
 The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muVHtautau (const double sqrt_s) const
 The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muVHWW (const double sqrt_s) const
 The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muVHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muVHZga (const double sqrt_s) const
 The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muVHZZ (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muVHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muWH (const double sqrt_s) const
 The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muWHbb (const double sqrt_s) const
 The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muWHgaga (const double sqrt_s) const
 The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muWHmumu (const double sqrt_s) const
 The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muWHtautau (const double sqrt_s) const
 The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muWHWW (const double sqrt_s) const
 The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muWHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muWHZga (const double sqrt_s) const
 The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muWHZZ (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muWHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double muZH (const double sqrt_s) const
 The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual double muZHbb (const double sqrt_s) const
 The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual double muZHgaga (const double sqrt_s) const
 The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual double muZHmumu (const double sqrt_s) const
 The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual double muZHtautau (const double sqrt_s) const
 The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual double muZHWW (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual double muZHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual double muZHZga (const double sqrt_s) const
 The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual double muZHZZ (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual double muZHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual double Mw () const
 The mass of the \(W\) boson, \(M_W\). More...
 
 NPSMEFTd6 (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false)
 Constructor. More...
 
virtual double obliqueS () const
 The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More...
 
virtual double obliqueT () const
 The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More...
 
virtual double obliqueU () const
 The oblique parameter \(U\). More...
 
virtual double obliqueW () const
 The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More...
 
virtual double obliqueY () const
 The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More...
 
virtual bool PostUpdate ()
 The post-update method for NPSMEFTd6. More...
 
virtual double ppZHprobe (const double sqrt_s) const
 The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More...
 
virtual bool setFlag (const std::string name, const bool value)
 A method to set a flag of NPSMEFTd6. More...
 
virtual double STXS_ggH0j (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_0_60 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_120_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH1j_pTH_60_120 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_0_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_0_60 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_120_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH2j_pTH_60_120 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_ggH_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual double STXS_qqHll_pTV_0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_150_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHll_pTV_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual double STXS_qqHlv_pTV_0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_0_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHlv_pTV_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual double STXS_qqHqq_pTj_200 (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_Rest (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_qqHqq_VHtopo (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual double STXS_ttHtH (const double sqrt_s) const
 The STXS bin \( ttH + tH \). More...
 
virtual double STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_Rest (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_WHqqHqq_VH2j (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_Rest (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double STXS_ZHqqHqq_VH2j (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual double xseeWW (const double sqrt_s) const
 Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More...
 
- Public Member Functions inherited from NPbase
virtual double A_f (const Particle f) const
 The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More...
 
virtual double AFB (const Particle f) const
 The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More...
 
virtual double BR_Zf (const Particle f) const
 The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More...
 
virtual double cbminuscc () const
 
virtual double cbminusctau () const
 
virtual double ccminusctau () const
 
virtual double cgaplusct () const
 
virtual double cgminuscga () const
 
virtual double cgplusct () const
 
virtual double cVpluscb () const
 
virtual double cVplusctau () const
 
virtual double deltaA_f (const Particle f) const
 The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More...
 
virtual double deltaAFB (const Particle f) const
 The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More...
 
virtual double deltaGamma_Z () const
 The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More...
 
virtual double deltaGamma_Zf (const Particle f) const
 The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
virtual double deltaGamma_Zhad () const
 The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More...
 
virtual double deltaN_nu () const
 The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More...
 
virtual double deltaR0_f (const Particle f) const
 The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
 
virtual double deltaR_inv () const
 The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More...
 
virtual double deltaSigmaHadron () const
 The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More...
 
virtual double deltaSin2thetaEff_e () const
 The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More...
 
virtual double deltaSin2thetaEff_mu () const
 The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More...
 
virtual gslpp::complex gA_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual double Gamma_had () const
 The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More...
 
virtual double Gamma_Z () const
 The total decay width of the \(Z\) boson, \(\Gamma_Z\). More...
 
virtual double Gamma_Zf (const Particle f) const
 The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More...
 
virtual StandardModel getTrueSM () const
 A method to return a StandardModel object from NPbase. More...
 
virtual gslpp::complex gV_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual gslpp::complex kappaZ_f (const Particle f) const
 The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More...
 
virtual double muggHgagaInt (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More...
 
virtual double muppHmumu (const double sqrt_s) const
 
virtual double muppHZga (const double sqrt_s) const
 
virtual double N_nu () const
 The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More...
 
 NPbase ()
 The default constructor. More...
 
virtual double R0_f (const Particle f) const
 The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
 
virtual double R_inv () const
 The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More...
 
virtual gslpp::complex rhoZ_f (const Particle f) const
 The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More...
 
virtual double sigma0_had () const
 The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More...
 
virtual double sin2thetaEff (const Particle f) const
 The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More...
 
virtual bool Update (const std::map< std::string, double > &DPars)
 The update method for NPbase. More...
 
virtual double UpperLimitZgammaA (const double sqrt_s) const
 
virtual double UpperLimitZgammaA13 (const double sqrt_s) const
 
virtual double UpperLimitZgammaC (const double sqrt_s) const
 
virtual double UpperLimitZgammaC13 (const double sqrt_s) const
 
- Public Member Functions inherited from StandardModel
double Ale (double mu, orders order, bool Nf_thr=true) const
 The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More...
 
double ale_OS (const double mu, orders order=FULLNLO) const
 The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More...
 
double alphaMz () const
 The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More...
 
double Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
 The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More...
 
double AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const
 
double Alstilde5 (const double mu) const
 The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More...
 
double Beta_e (int nm, unsigned int nf) const
 QED beta function coefficients - eq. (36) hep-ph/0512066. More...
 
double Beta_s (int nm, unsigned int nf) const
 QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More...
 
double c02 () const
 The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More...
 
virtual bool CheckFlags () const
 A method to check the sanity of the set of model flags. More...
 
bool checkSMparamsForEWPO ()
 A method to check whether the parameters relevant to the EWPO are updated. More...
 
double computeBrHtobb () const
 The Br \((H\to bb)\) in the Standard Model. More...
 
double computeBrHtocc () const
 The Br \((H\to cc)\) in the Standard Model. More...
 
double computeBrHtogaga () const
 The Br \((H\to\gamma\gamma)\) in the Standard Model. More...
 
double computeBrHtogg () const
 The Br \((H\to gg)\) in the Standard Model. More...
 
double computeBrHtomumu () const
 The Br \((H\to \mu\mu)\) in the Standard Model. More...
 
double computeBrHtoss () const
 The Br \((H\to ss)\) in the Standard Model. More...
 
double computeBrHtotautau () const
 The Br \((H\to \tau\tau)\) in the Standard Model. More...
 
double computeBrHtoWW () const
 The Br \((H\to WW)\) in the Standard Model. More...
 
double computeBrHtoZga () const
 The Br \((H\to Z\gamma)\) in the Standard Model. More...
 
double computeBrHtoZZ () const
 The Br \((H\to ZZ)\) in the Standard Model. More...
 
double computeBrHtoZZinv () const
 The Br \((H\to ZZ \to inv)\) in the Standard Model. More...
 
void ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const
 A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More...
 
void ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
 A method to collect \(\Delta\rho\) computed via subclasses. More...
 
double computeGammaHgaga_tt () const
 The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgaga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgaga_WW () const
 The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
double computeGammaHgg_bb () const
 The bottom loop contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHgg_tb () const
 The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHgg_tt () const
 The top loop contribution to \(H\to gg\) in the Standard Model. More...
 
double computeGammaHTotal () const
 The Higgs total width in the Standard Model. More...
 
double computeGammaHZga_tt () const
 The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
double computeGammaHZga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
double computeGammaHZga_WW () const
 The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [138]. More...
 
double computeSigmaggH (const double sqrt_s) const
 The ggH cross section in the Standard Model. More...
 
double computeSigmaggH_bb (const double sqrt_s) const
 The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmaggH_tb (const double sqrt_s) const
 The top-bottom interference contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmaggH_tt (const double sqrt_s) const
 The square of the top-quark contribution to the ggH cross section in the Standard Model. More...
 
double computeSigmattH (const double sqrt_s) const
 The ttH production cross section in the Standard Model. More...
 
double computeSigmaVBF (const double sqrt_s) const
 The VBF cross section in the Standard Model. More...
 
double computeSigmaWF (const double sqrt_s) const
 The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More...
 
double computeSigmaWH (const double sqrt_s) const
 The WH production cross section in the Standard Model. More...
 
double computeSigmaZF (const double sqrt_s) const
 The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More...
 
double computeSigmaZH (const double sqrt_s) const
 The ZH production cross section in the Standard Model. More...
 
double computeSigmaZWF (const double sqrt_s) const
 The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More...
 
virtual double cW2 () const
 
virtual double cW2 (const double Mw_i) const
 The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More...
 
double DeltaAlpha () const
 The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More...
 
double DeltaAlphaL5q () const
 The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More...
 
double DeltaAlphaLepton (const double s) const
 Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More...
 
double DeltaAlphaTop (const double s) const
 Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More...
 
virtual gslpp::complex deltaKappaZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More...
 
virtual double DeltaR () const
 The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More...
 
virtual double DeltaRbar () const
 The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More...
 
virtual gslpp::complex deltaRhoZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More...
 
virtual double epsilon1 () const
 The SM contribution to the epsilon parameter \(\varepsilon_1\). More...
 
virtual double epsilon2 () const
 The SM contribution to the epsilon parameter \(\varepsilon_2\). More...
 
virtual double epsilon3 () const
 The SM contribution to the epsilon parameter \(\varepsilon_3\). More...
 
virtual double epsilonb () const
 The SM contribution to the epsilon parameter \(\varepsilon_b\). More...
 
virtual double Gamma_inv () const
 The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More...
 
virtual double GammaZ (const Particle f) const
 The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More...
 
double getAle () const
 A get method to retrieve the fine-structure constant \(\alpha\). More...
 
double getAlsMz () const
 A get method to access the value of \(\alpha_s(M_Z)\). More...
 
virtual double getCBd () const
 The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More...
 
virtual double getCBs () const
 The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More...
 
virtual double getCCC1 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC2 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC3 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC4 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCCC5 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual double getCDMK () const
 The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More...
 
virtual double getCepsK () const
 The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More...
 
CKM getCKM () const
 A get method to retrieve the member object of type CKM. More...
 
double getDAle5Mz () const
 A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
 
double getDelGammaZ () const
 A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More...
 
double getDelMw () const
 A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More...
 
double getDelR0b () const
 A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
double getDelR0c () const
 A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
double getDelR0l () const
 A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
double getDelSigma0H () const
 A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More...
 
double getDelSin2th_b () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
double getDelSin2th_l () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
double getDelSin2th_q () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
std::string getFlagKappaZ () const
 A method to retrieve the model flag KappaZ. More...
 
std::string getFlagMw () const
 A method to retrieve the model flag Mw. More...
 
std::string getFlagRhoZ () const
 A method to retrieve the model flag RhoZ. More...
 
const FlavourgetFlavour () const
 
double getGF () const
 A get method to retrieve the Fermi constant \(G_\mu\). More...
 
int getIterationNo () const
 
Particle getLeptons (const QCD::lepton p) const
 A get method to retrieve the member object of a lepton. More...
 
virtual double getMHl () const
 A get method to retrieve the Higgs mass \(m_h\). More...
 
virtual double getmq (const QCD::quark q, const double mu) const
 
double getMuw () const
 A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More...
 
EWSMApproximateFormulaegetMyApproximateFormulae () const
 A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...
 
EWSMcachegetMyEWSMcache () const
 A get method to retrieve the member pointer of type EWSMcache. More...
 
LeptonFlavourgetMyLeptonFlavour () const
 
EWSMOneLoopEWgetMyOneLoopEW () const
 A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...
 
EWSMThreeLoopEWgetMyThreeLoopEW () const
 
EWSMThreeLoopEW2QCDgetMyThreeLoopEW2QCD () const
 
EWSMThreeLoopQCDgetMyThreeLoopQCD () const
 
EWSMTwoFermionsLEP2getMyTwoFermionsLEP2 () const
 A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...
 
EWSMTwoLoopEWgetMyTwoLoopEW () const
 
EWSMTwoLoopQCDgetMyTwoLoopQCD () const
 
double getMz () const
 A get method to access the mass of the \(Z\) boson \(M_Z\). More...
 
virtual double getPhiBd () const
 Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More...
 
virtual double getPhiBs () const
 Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More...
 
gslpp::matrix< gslpp::complexgetUPMNS () const
 A get method to retrieve the object of the PMNS matrix. More...
 
gslpp::matrix< gslpp::complexgetVCKM () const
 A get method to retrieve the CKM matrix. More...
 
gslpp::matrix< gslpp::complexgetYd () const
 A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More...
 
gslpp::matrix< gslpp::complexgetYe () const
 A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More...
 
gslpp::matrix< gslpp::complexgetYn () const
 A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More...
 
gslpp::matrix< gslpp::complexgetYu () const
 A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More...
 
virtual bool Init (const std::map< std::string, double > &DPars)
 A method to initialize the model parameters. More...
 
virtual bool InitializeModel ()
 A method to initialize the model. More...
 
bool IsFlagNoApproximateGammaZ () const
 A method to retrieve the model flag NoApproximateGammaZ. More...
 
bool IsFlagWithoutNonUniversalVC () const
 A method to retrieve the model flag WithoutNonUniversalVC. More...
 
virtual double LEP2AFBbottom (const double s) const
 
virtual double LEP2AFBcharm (const double s) const
 
virtual double LEP2AFBmu (const double s) const
 
virtual double LEP2AFBtau (const double s) const
 
virtual double LEP2Rbottom (const double s) const
 
virtual double LEP2Rcharm (const double s) const
 
virtual double LEP2sigmaBottom (const double s) const
 
virtual double LEP2sigmaCharm (const double s) const
 
virtual double LEP2sigmaHadron (const double s) const
 
virtual double LEP2sigmaMu (const double s) const
 
virtual double LEP2sigmaTau (const double s) const
 
virtual double Mw_tree () const
 The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More...
 
double MwbarFromMw (const double Mw) const
 A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...
 
double MwFromMwbar (const double Mwbar) const
 A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...
 
double Mzbar () const
 The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More...
 
virtual bool PreUpdate ()
 The pre-update method for StandardModel. More...
 
virtual double rho_GammaW (const Particle fi, const Particle fj) const
 EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More...
 
double s02 () const
 The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More...
 
void setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
 A set method to change the model flag CacheInStandardModel of StandardModel. More...
 
void setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)
 
bool setFlagSigmaForAFB (const bool flagSigmaForAFB_i)
 
bool setFlagSigmaForR (const bool flagSigmaForR_i)
 
virtual bool setFlagStr (const std::string name, const std::string value)
 A method to set a flag of StandardModel. More...
 
 StandardModel ()
 The default constructor. More...
 
double sW2 () const
 
virtual double sW2 (const double Mw_i) const
 The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More...
 
virtual double v () const
 The Higgs vacuum expectation value. More...
 
virtual ~StandardModel ()
 The default destructor. More...
 
- Public Member Functions inherited from QCD
double AboveTh (const double mu) const
 The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
void addParameters (std::vector< std::string > params_i)
 A method to add parameters that are specific to only one set of observables. More...
 
virtual double Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
 
double Als4 (const double mu) const
 The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More...
 
virtual double AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
 
double AlsOLD (const double mu, const orders order=FULLNLO) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
 
double AlsWithInit (const double mu, const double alsi, const double mu_i, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More...
 
double AlsWithLambda (const double mu, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More...
 
double BelowTh (const double mu) const
 The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
double Beta0 (const double nf) const
 The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta1 (const double nf) const
 The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta2 (const double nf) const
 The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
double Beta3 (const double nf) const
 The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
void CacheShift (double cache[][5], int n) const
 A member used to manage the caching for this class. More...
 
void CacheShift (int cache[][5], int n) const
 
orders FullOrder (orders order) const
 Return the FULLORDER enum corresponding to order. More...
 
double Gamma0 (const double nf) const
 The \(\gamma_0\) coefficient used to compute the running of a mass. More...
 
double Gamma1 (const double nf) const
 The \(\gamma_1\) coefficient used to compute the running of a mass. More...
 
double Gamma2 (const double nf) const
 The \(\gamma_2\) coefficient used to compute the running of a mass. More...
 
double getAlsM () const
 A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More...
 
BParameter getBBd () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More...
 
BParameter getBBs () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More...
 
BParameter getBD () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More...
 
BParameter getBK () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More...
 
BParameter getBKd1 () const
 
BParameter getBKd3 () const
 
double getCF () const
 A get method to access the Casimir factor of QCD. More...
 
double getMAls () const
 A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More...
 
Meson getMesons (const QCD::meson m) const
 A get method to access a meson as an object of the type Meson. More...
 
double getMtpole () const
 A get method to access the pole mass of the top quark. More...
 
double getMub () const
 A get method to access the threshold between five- and four-flavour theory in GeV. More...
 
double getMuc () const
 A get method to access the threshold between four- and three-flavour theory in GeV. More...
 
double getMut () const
 A get method to access the threshold between six- and five-flavour theory in GeV. More...
 
double getNc () const
 A get method to access the number of colours \(N_c\). More...
 
double getOptionalParameter (std::string name) const
 A method to get parameters that are specific to only one set of observables. More...
 
Particle getQuarks (const QCD::quark q) const
 A get method to access a quark as an object of the type Particle. More...
 
std::vector< std::string > getUnknownParameters ()
 A method to get the vector of the parameters that have been specified in the configuration file but not being used. More...
 
void initializeBParameter (std::string name_i) const
 A method to initialize B Parameter and the corresponding meson. More...
 
void initializeMeson (QCD::meson meson_i) const
 A method to initialize a meson. More...
 
double logLambda (const double nf, orders order) const
 Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More...
 
double Mbar2Mp (const double mbar, const orders order=FULLNNLO) const
 Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More...
 
double Mp2Mbar (const double mp, const orders order=FULLNNLO) const
 Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More...
 
double Mrun (const double mu, const double m, const orders order=FULLNNLO) const
 Computes a running quark mass \(m(\mu)\) from \(m(m)\). More...
 
double Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNNLO) const
 Runs a quark mass from \(\mu_i\) to \(\mu_f\). More...
 
double Mrun4 (const double mu_f, const double mu_i, const double m) const
 The running of a mass with the number of flavours \(n_f = 4\). More...
 
double MS2DRqmass (const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
double MS2DRqmass (const double MSscale, const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
double Nf (const double mu) const
 The number of active flavour at scale \(\mu\). More...
 
double NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
 Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More...
 
std::string orderToString (const orders order) const
 Converts an object of the enum type "orders" to the corresponding string. More...
 
 QCD ()
 Constructor. More...
 
void setNc (double Nc)
 A set method to change the number of colours \(N_c\). More...
 
void setOptionalParameter (std::string name, double value)
 A method to set the parameter value for the parameters that are specific to only one set of observables. More...
 
double Thresholds (const int i) const
 For accessing the active flavour threshold scales. More...
 
- Public Member Functions inherited from Model
void addMissingModelParameter (const std::string &missingParameterName)
 
std::vector< std::string > getmissingModelParameters ()
 
unsigned int getMissingModelParametersCount ()
 
std::string getModelName () const
 A method to fetch the name of the model. More...
 
const double & getModelParam (std::string name) const
 
bool isModelFWC_DF2 () const
 
bool isModelGeneralTHDM () const
 
bool isModelGeorgiMachacek () const
 
bool IsModelInitialized () const
 A method to check if the model is initialized. More...
 
bool isModelLinearized () const
 
bool isModelParam (std::string name) const
 
bool isModelSUSY () const
 
bool isModelTHDM () const
 
bool isModelTHDMW () const
 
bool IsUpdateError () const
 A method to check if there was any error in the model update process. More...
 
 Model ()
 The default constructor. More...
 
void raiseMissingModelParameterCount ()
 
void setModelFWC_DF2 ()
 
void setModelGeneralTHDM ()
 
void setModelGeorgiMachacek ()
 
void setModelInitialized (bool ModelInitialized)
 A set method to fix the failure or success of the initialization of the model. More...
 
void setModelLinearized (bool linearized=true)
 
void setModelName (const std::string name)
 A method to set the name of the model. More...
 
void setModelSUSY ()
 
void setModelTHDM ()
 
void setModelTHDMW ()
 
void setSliced (bool Sliced)
 
void setUpdateError (bool UpdateError)
 A set method to fix the update status as success or failure. More...
 
virtual ~Model ()
 The default destructor. More...
 

Static Public Attributes

static const int NNPSMEFTd6Vars = 506
 The number of the model parameters in NPSMEFTd6. More...
 
static const int NNPSMEFTd6Vars_LFU_QFU = 260
 The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities. More...
 
static const std::string NPSMEFTd6Vars [NNPSMEFTd6Vars]
 A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false. More...
 
static const std::string NPSMEFTd6Vars_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU]
 A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false. More...
 
static const std::string NPSMEFTd6VarsRot [NNPSMEFTd6Vars]
 A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true. More...
 
static const std::string NPSMEFTd6VarsRot_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU]
 A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true. More...
 
- Static Public Attributes inherited from StandardModel
static const double GeVminus2_to_nb = 389379.338
 
static const double Mw_error = 0.00001
 The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More...
 
static const int NSMvars = 26
 The number of the model parameters in StandardModel. More...
 
static const int NumSMParamsForEWPO = 33
 The number of the SM parameters that are relevant to the EW precision observables. More...
 
static std::string SMvars [NSMvars]
 A string array containing the labels of the model parameters in StandardModel. More...
 
- Static Public Attributes inherited from QCD
static const int NQCDvars = 11
 The number of model parameters in QCD. More...
 
static std::string QCDvars [NQCDvars]
 An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More...
 

Protected Member Functions

gslpp::complex CfB_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More...
 
gslpp::complex CfG_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More...
 
gslpp::complex CfH_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More...
 
gslpp::complex CfW_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More...
 
double CHF1_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More...
 
double CHF3_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More...
 
double CHf_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More...
 
gslpp::complex CHud_diag (const Particle u) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f. More...
 
virtual void setParameter (const std::string name, const double &value)
 A method to set the value of a parameter of the model. More...
 
- Protected Member Functions inherited from StandardModel
double AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const
 
double AFB_NoISR_q (const QCD::quark q_flavor, const double s) const
 
bool checkEWPOscheme (const std::string scheme) const
 A method to check if a given scheme name in string form is valid. More...
 
virtual void computeCKM ()
 The method to compute the CKM matrix. More...
 
virtual void computeYukawas ()
 The method to compute the Yukawa matrices. More...
 
double Delta_EWQCD (const QCD::quark q) const
 The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More...
 
double getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm133 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm167 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_charm207 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu130 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu136 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu161 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_mu207 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau130 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau136 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau161 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau172 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau183 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau189 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau192 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau196 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau200 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau202 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau205 (double x) const
 
double getIntegrand_AFBnumeratorWithISR_tau207 (double x) const
 
double getIntegrand_dsigmaBox_bottom130 (double x) const
 
double getIntegrand_dsigmaBox_bottom133 (double x) const
 
double getIntegrand_dsigmaBox_bottom136 (double x) const
 
double getIntegrand_dsigmaBox_bottom161 (double x) const
 
double getIntegrand_dsigmaBox_bottom167 (double x) const
 
double getIntegrand_dsigmaBox_bottom172 (double x) const
 
double getIntegrand_dsigmaBox_bottom183 (double x) const
 
double getIntegrand_dsigmaBox_bottom189 (double x) const
 
double getIntegrand_dsigmaBox_bottom192 (double x) const
 
double getIntegrand_dsigmaBox_bottom196 (double x) const
 
double getIntegrand_dsigmaBox_bottom200 (double x) const
 
double getIntegrand_dsigmaBox_bottom202 (double x) const
 
double getIntegrand_dsigmaBox_bottom205 (double x) const
 
double getIntegrand_dsigmaBox_bottom207 (double x) const
 
double getIntegrand_dsigmaBox_charm130 (double x) const
 
double getIntegrand_dsigmaBox_charm133 (double x) const
 
double getIntegrand_dsigmaBox_charm136 (double x) const
 
double getIntegrand_dsigmaBox_charm161 (double x) const
 
double getIntegrand_dsigmaBox_charm167 (double x) const
 
double getIntegrand_dsigmaBox_charm172 (double x) const
 
double getIntegrand_dsigmaBox_charm183 (double x) const
 
double getIntegrand_dsigmaBox_charm189 (double x) const
 
double getIntegrand_dsigmaBox_charm192 (double x) const
 
double getIntegrand_dsigmaBox_charm196 (double x) const
 
double getIntegrand_dsigmaBox_charm200 (double x) const
 
double getIntegrand_dsigmaBox_charm202 (double x) const
 
double getIntegrand_dsigmaBox_charm205 (double x) const
 
double getIntegrand_dsigmaBox_charm207 (double x) const
 
double getIntegrand_dsigmaBox_down130 (double x) const
 
double getIntegrand_dsigmaBox_down133 (double x) const
 
double getIntegrand_dsigmaBox_down136 (double x) const
 
double getIntegrand_dsigmaBox_down161 (double x) const
 
double getIntegrand_dsigmaBox_down167 (double x) const
 
double getIntegrand_dsigmaBox_down172 (double x) const
 
double getIntegrand_dsigmaBox_down183 (double x) const
 
double getIntegrand_dsigmaBox_down189 (double x) const
 
double getIntegrand_dsigmaBox_down192 (double x) const
 
double getIntegrand_dsigmaBox_down196 (double x) const
 
double getIntegrand_dsigmaBox_down200 (double x) const
 
double getIntegrand_dsigmaBox_down202 (double x) const
 
double getIntegrand_dsigmaBox_down205 (double x) const
 
double getIntegrand_dsigmaBox_down207 (double x) const
 
double getIntegrand_dsigmaBox_mu130 (double x) const
 
double getIntegrand_dsigmaBox_mu133 (double x) const
 
double getIntegrand_dsigmaBox_mu136 (double x) const
 
double getIntegrand_dsigmaBox_mu161 (double x) const
 
double getIntegrand_dsigmaBox_mu167 (double x) const
 
double getIntegrand_dsigmaBox_mu172 (double x) const
 
double getIntegrand_dsigmaBox_mu183 (double x) const
 
double getIntegrand_dsigmaBox_mu189 (double x) const
 
double getIntegrand_dsigmaBox_mu192 (double x) const
 
double getIntegrand_dsigmaBox_mu196 (double x) const
 
double getIntegrand_dsigmaBox_mu200 (double x) const
 
double getIntegrand_dsigmaBox_mu202 (double x) const
 
double getIntegrand_dsigmaBox_mu205 (double x) const
 
double getIntegrand_dsigmaBox_mu207 (double x) const
 
double getIntegrand_dsigmaBox_strange130 (double x) const
 
double getIntegrand_dsigmaBox_strange133 (double x) const
 
double getIntegrand_dsigmaBox_strange136 (double x) const
 
double getIntegrand_dsigmaBox_strange161 (double x) const
 
double getIntegrand_dsigmaBox_strange167 (double x) const
 
double getIntegrand_dsigmaBox_strange172 (double x) const
 
double getIntegrand_dsigmaBox_strange183 (double x) const
 
double getIntegrand_dsigmaBox_strange189 (double x) const
 
double getIntegrand_dsigmaBox_strange192 (double x) const
 
double getIntegrand_dsigmaBox_strange196 (double x) const
 
double getIntegrand_dsigmaBox_strange200 (double x) const
 
double getIntegrand_dsigmaBox_strange202 (double x) const
 
double getIntegrand_dsigmaBox_strange205 (double x) const
 
double getIntegrand_dsigmaBox_strange207 (double x) const
 
double getIntegrand_dsigmaBox_tau130 (double x) const
 
double getIntegrand_dsigmaBox_tau133 (double x) const
 
double getIntegrand_dsigmaBox_tau136 (double x) const
 
double getIntegrand_dsigmaBox_tau161 (double x) const
 
double getIntegrand_dsigmaBox_tau167 (double x) const
 
double getIntegrand_dsigmaBox_tau172 (double x) const
 
double getIntegrand_dsigmaBox_tau183 (double x) const
 
double getIntegrand_dsigmaBox_tau189 (double x) const
 
double getIntegrand_dsigmaBox_tau192 (double x) const
 
double getIntegrand_dsigmaBox_tau196 (double x) const
 
double getIntegrand_dsigmaBox_tau200 (double x) const
 
double getIntegrand_dsigmaBox_tau202 (double x) const
 
double getIntegrand_dsigmaBox_tau205 (double x) const
 
double getIntegrand_dsigmaBox_tau207 (double x) const
 
double getIntegrand_dsigmaBox_up130 (double x) const
 
double getIntegrand_dsigmaBox_up133 (double x) const
 
double getIntegrand_dsigmaBox_up136 (double x) const
 
double getIntegrand_dsigmaBox_up161 (double x) const
 
double getIntegrand_dsigmaBox_up167 (double x) const
 
double getIntegrand_dsigmaBox_up172 (double x) const
 
double getIntegrand_dsigmaBox_up183 (double x) const
 
double getIntegrand_dsigmaBox_up189 (double x) const
 
double getIntegrand_dsigmaBox_up192 (double x) const
 
double getIntegrand_dsigmaBox_up196 (double x) const
 
double getIntegrand_dsigmaBox_up200 (double x) const
 
double getIntegrand_dsigmaBox_up202 (double x) const
 
double getIntegrand_dsigmaBox_up205 (double x) const
 
double getIntegrand_dsigmaBox_up207 (double x) const
 
double getIntegrand_sigmaWithISR_bottom130 (double x) const
 
double getIntegrand_sigmaWithISR_bottom133 (double x) const
 
double getIntegrand_sigmaWithISR_bottom136 (double x) const
 
double getIntegrand_sigmaWithISR_bottom161 (double x) const
 
double getIntegrand_sigmaWithISR_bottom167 (double x) const
 
double getIntegrand_sigmaWithISR_bottom172 (double x) const
 
double getIntegrand_sigmaWithISR_bottom183 (double x) const
 
double getIntegrand_sigmaWithISR_bottom189 (double x) const
 
double getIntegrand_sigmaWithISR_bottom192 (double x) const
 
double getIntegrand_sigmaWithISR_bottom196 (double x) const
 
double getIntegrand_sigmaWithISR_bottom200 (double x) const
 
double getIntegrand_sigmaWithISR_bottom202 (double x) const
 
double getIntegrand_sigmaWithISR_bottom205 (double x) const
 
double getIntegrand_sigmaWithISR_bottom207 (double x) const
 
double getIntegrand_sigmaWithISR_charm130 (double x) const
 
double getIntegrand_sigmaWithISR_charm133 (double x) const
 
double getIntegrand_sigmaWithISR_charm136 (double x) const
 
double getIntegrand_sigmaWithISR_charm161 (double x) const
 
double getIntegrand_sigmaWithISR_charm167 (double x) const
 
double getIntegrand_sigmaWithISR_charm172 (double x) const
 
double getIntegrand_sigmaWithISR_charm183 (double x) const
 
double getIntegrand_sigmaWithISR_charm189 (double x) const
 
double getIntegrand_sigmaWithISR_charm192 (double x) const
 
double getIntegrand_sigmaWithISR_charm196 (double x) const
 
double getIntegrand_sigmaWithISR_charm200 (double x) const
 
double getIntegrand_sigmaWithISR_charm202 (double x) const
 
double getIntegrand_sigmaWithISR_charm205 (double x) const
 
double getIntegrand_sigmaWithISR_charm207 (double x) const
 
double getIntegrand_sigmaWithISR_down130 (double x) const
 
double getIntegrand_sigmaWithISR_down133 (double x) const
 
double getIntegrand_sigmaWithISR_down136 (double x) const
 
double getIntegrand_sigmaWithISR_down161 (double x) const
 
double getIntegrand_sigmaWithISR_down167 (double x) const
 
double getIntegrand_sigmaWithISR_down172 (double x) const
 
double getIntegrand_sigmaWithISR_down183 (double x) const
 
double getIntegrand_sigmaWithISR_down189 (double x) const
 
double getIntegrand_sigmaWithISR_down192 (double x) const
 
double getIntegrand_sigmaWithISR_down196 (double x) const
 
double getIntegrand_sigmaWithISR_down200 (double x) const
 
double getIntegrand_sigmaWithISR_down202 (double x) const
 
double getIntegrand_sigmaWithISR_down205 (double x) const
 
double getIntegrand_sigmaWithISR_down207 (double x) const
 
double getIntegrand_sigmaWithISR_mu130 (double x) const
 
double getIntegrand_sigmaWithISR_mu136 (double x) const
 
double getIntegrand_sigmaWithISR_mu161 (double x) const
 
double getIntegrand_sigmaWithISR_mu172 (double x) const
 
double getIntegrand_sigmaWithISR_mu183 (double x) const
 
double getIntegrand_sigmaWithISR_mu189 (double x) const
 
double getIntegrand_sigmaWithISR_mu192 (double x) const
 
double getIntegrand_sigmaWithISR_mu196 (double x) const
 
double getIntegrand_sigmaWithISR_mu200 (double x) const
 
double getIntegrand_sigmaWithISR_mu202 (double x) const
 
double getIntegrand_sigmaWithISR_mu205 (double x) const
 
double getIntegrand_sigmaWithISR_mu207 (double x) const
 
double getIntegrand_sigmaWithISR_strange130 (double x) const
 
double getIntegrand_sigmaWithISR_strange133 (double x) const
 
double getIntegrand_sigmaWithISR_strange136 (double x) const
 
double getIntegrand_sigmaWithISR_strange161 (double x) const
 
double getIntegrand_sigmaWithISR_strange167 (double x) const
 
double getIntegrand_sigmaWithISR_strange172 (double x) const
 
double getIntegrand_sigmaWithISR_strange183 (double x) const
 
double getIntegrand_sigmaWithISR_strange189 (double x) const
 
double getIntegrand_sigmaWithISR_strange192 (double x) const
 
double getIntegrand_sigmaWithISR_strange196 (double x) const
 
double getIntegrand_sigmaWithISR_strange200 (double x) const
 
double getIntegrand_sigmaWithISR_strange202 (double x) const
 
double getIntegrand_sigmaWithISR_strange205 (double x) const
 
double getIntegrand_sigmaWithISR_strange207 (double x) const
 
double getIntegrand_sigmaWithISR_tau130 (double x) const
 
double getIntegrand_sigmaWithISR_tau136 (double x) const
 
double getIntegrand_sigmaWithISR_tau161 (double x) const
 
double getIntegrand_sigmaWithISR_tau172 (double x) const
 
double getIntegrand_sigmaWithISR_tau183 (double x) const
 
double getIntegrand_sigmaWithISR_tau189 (double x) const
 
double getIntegrand_sigmaWithISR_tau192 (double x) const
 
double getIntegrand_sigmaWithISR_tau196 (double x) const
 
double getIntegrand_sigmaWithISR_tau200 (double x) const
 
double getIntegrand_sigmaWithISR_tau202 (double x) const
 
double getIntegrand_sigmaWithISR_tau205 (double x) const
 
double getIntegrand_sigmaWithISR_tau207 (double x) const
 
double getIntegrand_sigmaWithISR_up130 (double x) const
 
double getIntegrand_sigmaWithISR_up133 (double x) const
 
double getIntegrand_sigmaWithISR_up136 (double x) const
 
double getIntegrand_sigmaWithISR_up161 (double x) const
 
double getIntegrand_sigmaWithISR_up167 (double x) const
 
double getIntegrand_sigmaWithISR_up172 (double x) const
 
double getIntegrand_sigmaWithISR_up183 (double x) const
 
double getIntegrand_sigmaWithISR_up189 (double x) const
 
double getIntegrand_sigmaWithISR_up192 (double x) const
 
double getIntegrand_sigmaWithISR_up196 (double x) const
 
double getIntegrand_sigmaWithISR_up200 (double x) const
 
double getIntegrand_sigmaWithISR_up202 (double x) const
 
double getIntegrand_sigmaWithISR_up205 (double x) const
 
double getIntegrand_sigmaWithISR_up207 (double x) const
 
double Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
 
double Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const
 
double Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const
 
double Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const
 
double Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
 
double Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const
 
double m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const
 
double RAq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More...
 
double resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const
 A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double RVh () const
 The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More...
 
double RVq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More...
 
double SchemeToDouble (const std::string scheme) const
 A method to convert a given scheme name in string form into a floating-point number with double precision. More...
 
double sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const
 
double sigma_NoISR_q (const QCD::quark q_flavor, const double s) const
 
double taub () const
 Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More...
 
- Protected Member Functions inherited from QCD
double MassOfNf (int nf) const
 The Mbar mass of the heaviest quark in the theory with Nf active flavour. More...
 

Protected Attributes

double ai2G
 
double ai3G
 
double aiA
 
double aiB
 
double aiG
 
double aiH
 
double aiHB
 
double aiHd
 
double aiHe
 
double aiHL
 
double aiHQ
 
double aiHu
 
double aiHW
 
double aipHL
 
double aipHQ
 
double aiT
 
double aiu
 
double aiuG
 
double aiWW
 
double aleMz
 The em constant at Mz. More...
 
double BrHexo
 The branching ratio of exotic (not invisible) Higgs decays. More...
 
double BrHinv
 The branching ratio of invisible Higgs decays. More...
 
double C2B
 The dimension-6 operator coefficient \(C_{2W}\). More...
 
double C2BS
 The dimension-6 operator coefficient \(C_{2W}^{SILH}\). More...
 
double C2W
 The dimension-6 operator coefficient \(C_{2B}\). More...
 
double C2WS
 The dimension-6 operator coefficient \(C_{2B}^{SILH}\). More...
 
double CDB
 The dimension-6 operator coefficient \(C_{DB}\). More...
 
double CdB_11i
 The dimension-6 operator coefficient \((C_{dB})_{11}\) (imaginary part). More...
 
double CdB_11r
 The dimension-6 operator coefficient \((C_{dB})_{11}\) (real part). More...
 
double CdB_12i
 The dimension-6 operator coefficient \((C_{dB})_{12}\) (imaginary part). More...
 
double CdB_12r
 The dimension-6 operator coefficient \((C_{dB})_{12}\) (real part). More...
 
double CdB_13i
 The dimension-6 operator coefficient \((C_{dB})_{13}\) (imaginary part). More...
 
double CdB_13r
 The dimension-6 operator coefficient \((C_{dB})_{13}\) (real part). More...
 
double CdB_22i
 The dimension-6 operator coefficient \((C_{dB})_{22}\) (imaginary part). More...
 
double CdB_22r
 The dimension-6 operator coefficient \((C_{dB})_{22}\) (real part). More...
 
double CdB_23i
 The dimension-6 operator coefficient \((C_{dB})_{23}\) (imaginary part). More...
 
double CdB_23r
 The dimension-6 operator coefficient \((C_{dB})_{23}\) (real part). More...
 
double CdB_33i
 The dimension-6 operator coefficient \((C_{dB})_{33}\) (imaginary part). More...
 
double CdB_33r
 The dimension-6 operator coefficient \((C_{dB})_{33}\) (real part). More...
 
double CdG_11i
 The dimension-6 operator coefficient \((C_{dG})_{11}\) (imaginary part). More...
 
double CdG_11r
 The dimension-6 operator coefficient \((C_{dG})_{11}\) (real part). More...
 
double CdG_12i
 The dimension-6 operator coefficient \((C_{dG})_{12}\) (imaginary part). More...
 
double CdG_12r
 The dimension-6 operator coefficient \((C_{dG})_{12}\) (real part). More...
 
double CdG_13i
 The dimension-6 operator coefficient \((C_{dG})_{13}\) (imaginary part). More...
 
double CdG_13r
 The dimension-6 operator coefficient \((C_{dG})_{13}\) (real part). More...
 
double CdG_22i
 The dimension-6 operator coefficient \((C_{dG})_{22}\) (imaginary part). More...
 
double CdG_22r
 The dimension-6 operator coefficient \((C_{dG})_{22}\) (real part). More...
 
double CdG_23i
 The dimension-6 operator coefficient \((C_{dG})_{23}\) (imaginary part). More...
 
double CdG_23r
 The dimension-6 operator coefficient \((C_{dG})_{23}\) (real part). More...
 
double CdG_33i
 The dimension-6 operator coefficient \((C_{dG})_{33}\) (imaginary part). More...
 
double CdG_33r
 The dimension-6 operator coefficient \((C_{dG})_{33}\) (real part). More...
 
double CdH_11i
 The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part). More...
 
double CdH_11r
 The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part). More...
 
double CdH_12i
 The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part). More...
 
double CdH_12r
 The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part). More...
 
double CdH_13i
 The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part). More...
 
double CdH_13r
 The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part). More...
 
double CdH_22i
 The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part). More...
 
double CdH_22r
 The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part). More...
 
double CdH_23i
 The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part). More...
 
double CdH_23r
 The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part). More...
 
double CdH_33i
 The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part). More...
 
double CdH_33r
 The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part). More...
 
double CDHB
 The dimension-6 operator coefficient \(C_{DHB}\). More...
 
double CDHW
 The dimension-6 operator coefficient \(C_{DHW}\). More...
 
double CDW
 The dimension-6 operator coefficient \(C_{DW}\). More...
 
double CdW_11i
 The dimension-6 operator coefficient \((C_{dW})_{11}\) (imaginary part). More...
 
double CdW_11r
 The dimension-6 operator coefficient \((C_{dW})_{11}\) (real part). More...
 
double CdW_12i
 The dimension-6 operator coefficient \((C_{dW})_{12}\) (imaginary part). More...
 
double CdW_12r
 The dimension-6 operator coefficient \((C_{dW})_{12}\) (real part). More...
 
double CdW_13i
 The dimension-6 operator coefficient \((C_{dW})_{13}\) (imaginary part). More...
 
double CdW_13r
 The dimension-6 operator coefficient \((C_{dW})_{13}\) (real part). More...
 
double CdW_22i
 The dimension-6 operator coefficient \((C_{dW})_{22}\) (imaginary part). More...
 
double CdW_22r
 The dimension-6 operator coefficient \((C_{dW})_{22}\) (real part). More...
 
double CdW_23i
 The dimension-6 operator coefficient \((C_{dW})_{23}\) (imaginary part). More...
 
double CdW_23r
 The dimension-6 operator coefficient \((C_{dW})_{23}\) (real part). More...
 
double CdW_33i
 The dimension-6 operator coefficient \((C_{dW})_{33}\) (imaginary part). More...
 
double CdW_33r
 The dimension-6 operator coefficient \((C_{dW})_{33}\) (real part). More...
 
double CeB_11i
 The dimension-6 operator coefficient \((C_{eB})_{11}\) (imaginary part). More...
 
double CeB_11r
 The dimension-6 operator coefficient \((C_{eB})_{11}\) (real part). More...
 
double CeB_12i
 The dimension-6 operator coefficient \((C_{eB})_{12}\) (imaginary part). More...
 
double CeB_12r
 The dimension-6 operator coefficient \((C_{eB})_{12}\) (real part). More...
 
double CeB_13i
 The dimension-6 operator coefficient \((C_{eB})_{13}\) (imaginary part). More...
 
double CeB_13r
 The dimension-6 operator coefficient \((C_{eB})_{13}\) (real part). More...
 
double CeB_22i
 The dimension-6 operator coefficient \((C_{eB})_{22}\) (imaginary part). More...
 
double CeB_22r
 The dimension-6 operator coefficient \((C_{eB})_{22}\) (real part). More...
 
double CeB_23i
 The dimension-6 operator coefficient \((C_{eB})_{23}\) (imaginary part). More...
 
double CeB_23r
 The dimension-6 operator coefficient \((C_{eB})_{23}\) (real part). More...
 
double CeB_33i
 The dimension-6 operator coefficient \((C_{eB})_{33}\) (imaginary part). More...
 
double CeB_33r
 The dimension-6 operator coefficient \((C_{eB})_{33}\) (real part). More...
 
double Ced_1111
 
double Ced_1122
 
double Ced_1123
 
double Ced_1132
 
double Ced_1133
 
double Ced_2211
 
double Ced_2223
 
double Ced_2232
 
double Ced_3311
 
double Ced_3323
 
double Ced_3332
 
double Cee_1111
 
double Cee_1122
 
double Cee_1133
 
double Cee_2211
 
double Cee_3311
 
double CeH_11i
 The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part). More...
 
double CeH_11r
 The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part). More...
 
double CeH_12i
 The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part). More...
 
double CeH_12r
 The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part). More...
 
double CeH_13i
 The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part). More...
 
double CeH_13r
 The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part). More...
 
double CeH_22i
 The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part). More...
 
double CeH_22r
 The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part). More...
 
double CeH_23i
 The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part). More...
 
double CeH_23r
 The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part). More...
 
double CeH_33i
 The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part). More...
 
double CeH_33r
 The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part). More...
 
double Ceu_1111
 
double Ceu_1122
 
double Ceu_1133
 
double Ceu_2211
 
double Ceu_2233
 
double Ceu_3311
 
double CeW_11i
 The dimension-6 operator coefficient \((C_{eW})_{11}\) (imaginary part). More...
 
double CeW_11r
 The dimension-6 operator coefficient \((C_{eW})_{11}\) (real part). More...
 
double CeW_12i
 The dimension-6 operator coefficient \((C_{eW})_{12}\) (imaginary part). More...
 
double CeW_12r
 The dimension-6 operator coefficient \((C_{eW})_{12}\) (real part). More...
 
double CeW_13i
 The dimension-6 operator coefficient \((C_{eW})_{13}\) (imaginary part). More...
 
double CeW_13r
 The dimension-6 operator coefficient \((C_{eW})_{13}\) (real part). More...
 
double CeW_22i
 The dimension-6 operator coefficient \((C_{eW})_{22}\) (imaginary part). More...
 
double CeW_22r
 The dimension-6 operator coefficient \((C_{eW})_{22}\) (real part). More...
 
double CeW_23i
 The dimension-6 operator coefficient \((C_{eW})_{23}\) (imaginary part). More...
 
double CeW_23r
 The dimension-6 operator coefficient \((C_{eW})_{23}\) (real part). More...
 
double CeW_33i
 The dimension-6 operator coefficient \((C_{eW})_{33}\) (imaginary part). More...
 
double CeW_33r
 The dimension-6 operator coefficient \((C_{eW})_{33}\) (real part). More...
 
double CG
 The dimension-6 operator coefficient \(C_{G}\). More...
 
double CH
 The dimension-6 operator coefficient \(C_{H}\). More...
 
double CHB
 The dimension-6 operator coefficient \(C_{HB}\). More...
 
double CHbox
 The dimension-6 operator coefficient \(C_{H\Box}\). More...
 
double CHD
 The dimension-6 operator coefficient \(C_{HD}\). More...
 
double CHd_11
 The dimension-6 operator coefficient \((C_{Hd})_{11}\). More...
 
double CHd_12i
 The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part). More...
 
double CHd_12r
 The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part). More...
 
double CHd_13i
 The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part). More...
 
double CHd_13r
 The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part). More...
 
double CHd_22
 The dimension-6 operator coefficient \((C_{Hd})_{22}\). More...
 
double CHd_23i
 The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part). More...
 
double CHd_23r
 The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part). More...
 
double CHd_33
 The dimension-6 operator coefficient \((C_{Hd})_{33}\). More...
 
double CHe_11
 The dimension-6 operator coefficient \((C_{He})_{11}\). More...
 
double CHe_12i
 The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part). More...
 
double CHe_12r
 The dimension-6 operator coefficient \((C_{He})_{12}\) (real part). More...
 
double CHe_13i
 The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part). More...
 
double CHe_13r
 The dimension-6 operator coefficient \((C_{He})_{13}\) (real part). More...
 
double CHe_22
 The dimension-6 operator coefficient \((C_{He})_{22}\). More...
 
double CHe_23i
 The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part). More...
 
double CHe_23r
 The dimension-6 operator coefficient \((C_{He})_{23}\) (real part). More...
 
double CHe_33
 The dimension-6 operator coefficient \((C_{He})_{33}\). More...
 
double CHG
 The dimension-6 operator coefficient \(C_{HG}\). More...
 
double CHL1_11
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More...
 
double CHL1_12i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More...
 
double CHL1_12r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More...
 
double CHL1_13i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More...
 
double CHL1_13r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More...
 
double CHL1_22
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More...
 
double CHL1_23i
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More...
 
double CHL1_23r
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More...
 
double CHL1_33
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More...
 
double CHL3_11
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More...
 
double CHL3_12i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
 
double CHL3_12r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More...
 
double CHL3_13i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
 
double CHL3_13r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More...
 
double CHL3_22
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More...
 
double CHL3_23i
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
 
double CHL3_23r
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More...
 
double CHL3_33
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More...
 
double CHQ1_11
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More...
 
double CHQ1_12i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More...
 
double CHQ1_12r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More...
 
double CHQ1_13i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More...
 
double CHQ1_13r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More...
 
double CHQ1_22
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More...
 
double CHQ1_23i
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More...
 
double CHQ1_23r
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More...
 
double CHQ1_33
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More...
 
double CHQ3_11
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More...
 
double CHQ3_12i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More...
 
double CHQ3_12r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More...
 
double CHQ3_13i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More...
 
double CHQ3_13r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More...
 
double CHQ3_22
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More...
 
double CHQ3_23i
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More...
 
double CHQ3_23r
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More...
 
double CHQ3_33
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More...
 
double cHSM
 Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More...
 
double CHu_11
 The dimension-6 operator coefficient \((C_{Hu})_{11}\). More...
 
double CHu_12i
 The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part). More...
 
double CHu_12r
 The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part). More...
 
double CHu_13i
 The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part). More...
 
double CHu_13r
 The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part). More...
 
double CHu_22
 The dimension-6 operator coefficient \((C_{Hu})_{22}\). More...
 
double CHu_23i
 The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part). More...
 
double CHu_23r
 The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part). More...
 
double CHu_33
 The dimension-6 operator coefficient \((C_{Hu})_{33}\). More...
 
double CHud_11i
 The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part). More...
 
double CHud_11r
 The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part). More...
 
double CHud_12i
 The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part). More...
 
double CHud_12r
 The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part). More...
 
double CHud_13i
 The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part). More...
 
double CHud_13r
 The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part). More...
 
double CHud_22i
 The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part). More...
 
double CHud_22r
 The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part). More...
 
double CHud_23i
 The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part). More...
 
double CHud_23r
 The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part). More...
 
double CHud_33i
 The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part). More...
 
double CHud_33r
 The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part). More...
 
double CHW
 The dimension-6 operator coefficient \(C_{HW}\). More...
 
double CHWB
 The dimension-6 operator coefficient \(C_{HWB}\). More...
 
double CHWHB_gaga
 The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\). More...
 
double CHWHB_gagaorth
 The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\). More...
 
double CidH_11r
 
double CidH_22r
 
double CidH_33r
 
double CiDHB
 
double CiDHW
 
double CieH_11r
 
double CieH_22r
 
double CieH_33r
 
double CiH
 
double CiHB
 
double CiHbox
 
double CiHD
 
double CiHd_11
 
double CiHd_22
 
double CiHd_33
 
double CiHe_11
 
double CiHe_22
 
double CiHe_33
 
double CiHL1_11
 
double CiHL1_22
 
double CiHL1_33
 
double CiHL3_11
 
double CiHL3_22
 
double CiHL3_33
 
double CiHQ1_11
 
double CiHQ1_22
 
double CiHQ1_33
 
double CiHQ3_11
 
double CiHQ3_22
 
double CiHQ3_33
 
double CiHu_11
 
double CiHu_22
 
double CiHu_33
 
double CiHW
 
double CiHWB
 
double CiLL_1221
 
double CiLL_2112
 
double CiuB_11r
 
double CiuB_22r
 
double CiuB_33r
 
double CiuG_11r
 
double CiuG_22r
 
double CiuG_33r
 
double CiuH_11r
 
double CiuH_22r
 
double CiuH_33r
 
double CiuW_11r
 
double CiuW_22r
 
double CiuW_33r
 
double CiW
 
double CLd_1111
 
double CLd_1122
 
double CLd_1123
 
double CLd_1132
 
double CLd_1133
 
double CLd_2211
 
double CLd_2223
 
double CLd_2232
 
double CLd_3311
 
double CLd_3323
 
double CLd_3332
 
double CLe_1111
 
double CLe_1122
 
double CLe_1133
 
double CLe_2211
 
double CLe_3311
 
double CLedQ_11
 
double CLedQ_22
 
double cLH3d62
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More...
 
double cLHd6
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More...
 
double CLL_1111
 
double CLL_1122
 
double CLL_1133
 
double CLL_1221
 
double CLL_1331
 
double CLL_2112
 
double CLL_2211
 
double CLL_3113
 
double CLL_3311
 
double CLQ1_1111
 
double CLQ1_1122
 
double CLQ1_1123
 
double CLQ1_1132
 
double CLQ1_1133
 
double CLQ1_1221
 
double CLQ1_1331
 
double CLQ1_2112
 
double CLQ1_2211
 
double CLQ1_2223
 
double CLQ1_2232
 
double CLQ1_3113
 
double CLQ1_3311
 
double CLQ1_3323
 
double CLQ1_3332
 
double CLQ3_1111
 
double CLQ3_1122
 
double CLQ3_1123
 
double CLQ3_1132
 
double CLQ3_1133
 
double CLQ3_1221
 
double CLQ3_1331
 
double CLQ3_2112
 
double CLQ3_2211
 
double CLQ3_2223
 
double CLQ3_2232
 
double CLQ3_3113
 
double CLQ3_3311
 
double CLQ3_3323
 
double CLQ3_3332
 
double CLu_1111
 
double CLu_1122
 
double CLu_1133
 
double CLu_2211
 
double CLu_2233
 
double CLu_3311
 
double CpLedQ_11
 
double CpLedQ_22
 
double CQe_1111
 
double CQe_1122
 
double CQe_1133
 
double CQe_2211
 
double CQe_2311
 
double CQe_2322
 
double CQe_2333
 
double CQe_3211
 
double CQe_3222
 
double CQe_3233
 
double CQe_3311
 
double CT
 The dimension-6 operator coefficient \(C_{T}\). More...
 
double CuB_11i
 The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More...
 
double CuB_11r
 The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More...
 
double CuB_12i
 The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More...
 
double CuB_12r
 The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More...
 
double CuB_13i
 The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More...
 
double CuB_13r
 The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More...
 
double CuB_22i
 The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More...
 
double CuB_22r
 The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More...
 
double CuB_23i
 The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More...
 
double CuB_23r
 The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More...
 
double CuB_33i
 The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More...
 
double CuB_33r
 The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More...
 
double CuG_11i
 The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More...
 
double CuG_11r
 The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More...
 
double CuG_12i
 The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More...
 
double CuG_12r
 The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More...
 
double CuG_13i
 The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More...
 
double CuG_13r
 The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More...
 
double CuG_22i
 The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More...
 
double CuG_22r
 The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More...
 
double CuG_23i
 The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More...
 
double CuG_23r
 The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More...
 
double CuG_33i
 The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More...
 
double CuG_33r
 The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). More...
 
double CuH_11i
 The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part). More...
 
double CuH_11r
 The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part). More...
 
double CuH_12i
 The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part). More...
 
double CuH_12r
 The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part). More...
 
double CuH_13i
 The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part). More...
 
double CuH_13r
 The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part). More...
 
double CuH_22i
 The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part). More...
 
double CuH_22r
 The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part). More...
 
double CuH_23i
 The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part). More...
 
double CuH_23r
 The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part). More...
 
double CuH_33i
 The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part). More...
 
double CuH_33r
 The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part). More...
 
double CuW_11i
 The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More...
 
double CuW_11r
 The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More...
 
double CuW_12i
 The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More...
 
double CuW_12r
 The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More...
 
double CuW_13i
 The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More...
 
double CuW_13r
 The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More...
 
double CuW_22i
 The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More...
 
double CuW_22r
 The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More...
 
double CuW_23i
 The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More...
 
double CuW_23r
 The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More...
 
double CuW_33i
 The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More...
 
double CuW_33r
 The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More...
 
double CW
 The dimension-6 operator coefficient \(C_{W}\). More...
 
double cW2_tree
 The square of the tree level values for the cosine of the weak angle. More...
 
double cW_tree
 The tree level values for the cosine of the weak angle. More...
 
double delta_AA
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_AZ
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_h
 Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More...
 
double delta_ZZ
 Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More...
 
double dg1Z
 Independent contribution to aTGC. More...
 
double dGammaHTotR1
 
double dGammaHTotR2
 
double dKappaga
 Independent contribution to aTGC.
More...
 
double dZH
 Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization. More...
 
double eeettHint
 Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeettHpar
 Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeeWBFint
 Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeWBFpar
 Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeZHint
 Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeeZHpar
 Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeMz
 The em coupling at Mz. More...
 
double eeMz2
 The em coupling squared (at Mz). More...
 
double eepWBFint
 Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More...
 
double eepWBFpar
 Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
More...
 
double eepZBFint
 Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More...
 
double eepZBFpar
 Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More...
 
double eggFHbb
 
double eggFHgaga
 
double eggFHmumu
 Total relative theoretical error in \(gg \to H \to X\).
More...
 
double eggFHtautau
 
double eggFHWW
 
double eggFHZga
 
double eggFHZZ
 
double eggFint
 Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eggFpar
 Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eHbbint
 Intrinsic relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHbbpar
 Parametric relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHccint
 Intrinsic relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHccpar
 Parametric relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHgagaint
 Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHgagapar
 Parametric relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHggint
 Intrinsic relative theoretical error in \(H \to g g\). More...
 
double eHggpar
 Parametric relative theoretical error in \(H \to g g\). More...
 
double eHmumuint
 Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHmumupar
 Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHtautauint
 Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHtautaupar
 Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHwidth
 Total relative theoretical error in the Higgs width. More...
 
double eHWWint
 Intrinsic relative theoretical error in \(H \to W W\). More...
 
double eHWWpar
 Parametric relative theoretical error in \(H \to W W\). More...
 
double eHZgaint
 Intrinsic relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZgapar
 Parametric relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZZint
 Intrinsic relative theoretical error in \(H \to Z Z\). More...
 
double eHZZpar
 Parametric relative theoretical error in \(H \to Z Z\). More...
 
double ettH_1314_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV). More...
 
double ettH_1314_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV). More...
 
double ettH_1314_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV). More...
 
double ettH_1314_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV). More...
 
double ettH_2_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV). More...
 
double ettH_2_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV). More...
 
double ettH_2_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV). More...
 
double ettH_2_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV). More...
 
double ettH_78_DeltagHt
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More...
 
double ettH_78_G
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV). More...
 
double ettH_78_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV). More...
 
double ettH_78_uG_33r
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV). More...
 
double ettHbb
 
double ettHgaga
 
double ettHint
 Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double ettHmumu
 Total relative theoretical error in \(pp \to ttH \to tt X\). More...
 
double ettHpar
 Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double ettHtautau
 
double ettHWW
 
double ettHZga
 
double ettHZZ
 
double eVBF_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV). More...
 
double eVBF_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV). More...
 
double eVBF_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HG
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBF_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV). More...
 
double eVBFHbb
 
double eVBFHgaga
 
double eVBFHinv
 
double eVBFHmumu
 Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).
More...
 
double eVBFHtautau
 
double eVBFHWW
 
double eVBFHZga
 
double eVBFHZZ
 
double eVBFint
 Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eVBFpar
 Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eVHinv
 Total relative theoretical error in \(pp \to X H \to X + invisible\). More...
 
double eWH_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV). More...
 
double eWH_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV). More...
 
double eWH_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV). More...
 
double eWH_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV). More...
 
double eWH_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV). More...
 
double eWH_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV). More...
 
double eWH_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV). More...
 
double eWH_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV). More...
 
double eWH_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWH_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV). More...
 
double eWHbb
 
double eWHgaga
 
double eWHint
 Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eWHmumu
 Total relative theoretical error in \(pp \to WH \to W X\).
More...
 
double eWHpar
 Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eWHtautau
 
double eWHWW
 
double eWHZga
 
double eWHZZ
 
double eZH_1314_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_1314_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV). More...
 
double eZH_2_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_2_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV). More...
 
double eZH_78_DeltaGF
 Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_DHB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_DHW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hbox
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HD
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hd_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HQ1_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HQ3_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_Hu_11
 Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HW
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZH_78_HWB
 Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV). More...
 
double eZHbb
 
double eZHgaga
 
double eZHint
 Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double eZHmumu
 Total relative theoretical error in \(pp \to ZH \to Z X\). More...
 
double eZHpar
 Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double eZHtautau
 
double eZHWW
 
double eZHZga
 
double eZHZZ
 
double g1_tree
 The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole). More...
 
double g2_tree
 The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole). More...
 
double g3_tree
 The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole). More...
 
double GammaHTotR
 NP contributions and Total to Higgs width ratio with SM. More...
 
double gZdL
 
double gZdR
 The tree level value of the \(Z\bar{d}d\) couplings in the SM. More...
 
double gZlL
 
double gZlR
 The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM. More...
 
double gZuL
 
double gZuR
 The tree level value of the \(Z\bar{u}u\) couplings in the SM. More...
 
double gZvL
 The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM. More...
 
double Lambda_NP
 The new physics scale [GeV]. More...
 
double lambdaH_tree
 The SM tree level value of the scalar quartic coupling in the potential. More...
 
double LambdaNP2
 The square of the new physics scale [GeV \(^2\)]. More...
 
double lambZ
 Independent contribution to aTGC. More...
 
Matching< NPSMEFTd6Matching, NPSMEFTd6NPSMEFTd6M
 
double sW2_tree
 The square of the tree level values for the sine of the weak angle. More...
 
double sW_tree
 The tree level values for the sine of the weak angle. More...
 
double UevL
 The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.) More...
 
double v2
 The square of the EW vev. More...
 
double v2_over_LambdaNP2
 The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). More...
 
double VudL
 The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.) More...
 
double Yukb
 SM d-quark Yukawas. More...
 
double Yukc
 
double Yukd
 
double Yuke
 
double Yukmu
 
double Yuks
 
double Yukt
 SM u-quark Yukawas. More...
 
double Yuktau
 SM lepton Yukawas. More...
 
double Yuku
 
- Protected Attributes inherited from NPbase
StandardModel trueSM
 
- Protected Attributes inherited from StandardModel
double A
 The CKM parameter \(A\) in the Wolfenstein parameterization. More...
 
double ale
 The fine-structure constant \(\alpha\). More...
 
double alpha21
 
double alpha31
 
double AlsMz
 The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More...
 
bool bSigmaForAFB
 
bool bSigmaForR
 
double dAle5Mz
 The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
 
double delGammaZ
 The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More...
 
double delMw
 The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More...
 
double delR0b
 The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
double delR0c
 The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
double delR0l
 The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
double delsigma0H
 The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More...
 
double delSin2th_b
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
double delSin2th_l
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
double delSin2th_q
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
double delta
 
double etab
 The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More...
 
bool flag_order [orders_EW_size]
 An array of internal flags controlling the inclusions of higher-order corrections. More...
 
bool flagLEP2 [NUMofLEP2RCs]
 
double gamma
 \(\gamma \) used as an input for FlagWolfenstein = FALSE More...
 
double GF
 The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More...
 
double lambda
 The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More...
 
Particle leptons [6]
 An array of Particle objects for the leptons. More...
 
double mHl
 The Higgs mass \(m_h\) in GeV. More...
 
double muw
 A matching scale \(\mu_W\) around the weak scale in GeV. More...
 
CKM myCKM
 An object of type CKM. More...
 
PMNS myPMNS
 
double Mz
 The mass of the \(Z\) boson in GeV. More...
 
bool requireCKM
 An internal flag to control whether the CKM matrix has to be recomputed. More...
 
bool requireYe
 An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...
 
bool requireYn
 An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...
 
double rhob
 The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More...
 
double s12
 
double s13
 
double s23
 
Flavour SMFlavour
 An object of type Flavour. More...
 
Matching< StandardModelMatching, StandardModelSMM
 An object of type Matching. More...
 
double Vcb
 \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vub
 \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vus
 \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
gslpp::matrix< gslpp::complexYd
 The Yukawa matrix of the down-type quarks. More...
 
gslpp::matrix< gslpp::complexYe
 The Yukawa matrix of the charged leptons. More...
 
gslpp::matrix< gslpp::complexYn
 The Yukawa matrix of the neutrinos. More...
 
gslpp::matrix< gslpp::complexYu
 The Yukawa matrix of the up-type quarks. More...
 
- Protected Attributes inherited from QCD
double AlsM
 The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More...
 
double CA
 
double CF
 
bool computemt
 Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More...
 
double dAdA_NA
 
double dFdA_NA
 
double dFdF_NA
 
double MAls
 The mass scale in GeV at which the strong coupling measurement is provided. More...
 
double mtpole
 The pole mass of the top quark. More...
 
double mub
 The threshold between five- and four-flavour theory in GeV. More...
 
double muc
 The threshold between four- and three-flavour theory in GeV. More...
 
double mut
 The threshold between six- and five-flavour theory in GeV. More...
 
double NA
 
double Nc
 The number of colours. More...
 
Particle quarks [6]
 The vector of all SM quarks. More...
 
bool requireYd
 Switch for generating the Yukawa couplings to the down-type quarks. More...
 
bool requireYu
 Switch for generating the Yukawa couplings to the up-type quarks. More...
 
double TF
 
- Protected Attributes inherited from Model
bool isSliced
 A boolean set to true if the current istance is a slice of an extended object. More...
 
std::map< std::string, std::reference_wrapper< const double > > ModelParamMap
 
bool UpdateError
 A boolean set to false if update is successful. More...
 

Private Attributes

bool FlagFlavU3OfX
 A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients. More...
 
bool FlagHiggsSM
 A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. More...
 
const bool FlagLeptonUniversal
 An internal boolean flag that is true if assuming lepton flavour universality. More...
 
bool FlagLoopH3d6Quad
 A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. More...
 
bool FlagLoopHd6
 A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. More...
 
bool FlagPartialQFU
 A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators. More...
 
bool FlagQuadraticTerms
 A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More...
 
const bool FlagQuarkUniversal
 An internal boolean flag that is true if assuming quark flavour universality. More...
 
bool FlagRotateCHWCHB
 A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB. More...
 
bool FlagUnivOfX
 A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively). More...
 
gsl_integration_cquad_workspace * w_WW
 

Additional Inherited Members

- Public Types inherited from StandardModel
enum  LEP2RCs { Weak = 0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs }
 
enum  orders_EW { EW1 = 0, EW1QCD1, EW1QCD2, EW2, EW2QCD1, EW3, orders_EW_size }
 An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More...
 
- Public Types inherited from QCD
enum  lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU, NOLEPTON }
 An enum type for leptons. More...
 
enum  meson { P_0, P_P, K_0, K_P, D_0, D_P, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, D_star_P, RHO, RHO_P, OMEGA, MESON_END }
 An enum type for mesons. More...
 
enum  quark { UP, DOWN, CHARM, STRANGE, TOP, BOTTOM }
 An enum type for quarks. More...
 

Constructor & Destructor Documentation

◆ NPSMEFTd6()

NPSMEFTd6::NPSMEFTd6 ( const bool  FlagLeptonUniversal_in = false,
const bool  FlagQuarkUniversal_in = false 
)

Constructor.

Parameters
[in]FlagLeptonUniversal_inan internal boolean flag that is true if assuming lepton flavour universality
[in]FlagQuarkUniversal_inan internal boolean flag that is true if assuming quark flavour universality

Definition at line 304 of file NPSMEFTd6.cpp.

305 : NPbase(), NPSMEFTd6M(*this), FlagLeptonUniversal(FlagLeptonUniversal_in), FlagQuarkUniversal(FlagQuarkUniversal_in)
306 {
309  throw std::runtime_error("Invalid arguments for NPSMEFTd6::NPSMEFTd6()");
310 
311  FlagQuadraticTerms = false;
312  FlagRotateCHWCHB = false;
313  FlagPartialQFU = false;
314  FlagFlavU3OfX = false;
315  FlagUnivOfX = false;
316  FlagHiggsSM = false;
317  FlagLoopHd6 = false;
318  FlagLoopH3d6Quad = false;
320 
321  w_WW = gsl_integration_cquad_workspace_alloc(100);
322 
324 
325  ModelParamMap.insert(std::make_pair("CG", std::cref(CG)));
326  ModelParamMap.insert(std::make_pair("CW", std::cref(CW)));
327  ModelParamMap.insert(std::make_pair("C2B", std::cref(C2B)));
328  ModelParamMap.insert(std::make_pair("C2W", std::cref(C2W)));
329  ModelParamMap.insert(std::make_pair("C2BS", std::cref(C2BS)));
330  ModelParamMap.insert(std::make_pair("C2WS", std::cref(C2WS)));
331  ModelParamMap.insert(std::make_pair("CHG", std::cref(CHG)));
332  ModelParamMap.insert(std::make_pair("CHW", std::cref(CHW)));
333  ModelParamMap.insert(std::make_pair("CHB", std::cref(CHB)));
334  ModelParamMap.insert(std::make_pair("CHWHB_gaga", std::cref(CHWHB_gaga)));
335  ModelParamMap.insert(std::make_pair("CHWHB_gagaorth", std::cref(CHWHB_gagaorth)));
336  ModelParamMap.insert(std::make_pair("CDHB", std::cref(CDHB)));
337  ModelParamMap.insert(std::make_pair("CDHW", std::cref(CDHW)));
338  ModelParamMap.insert(std::make_pair("CDB", std::cref(CDB)));
339  ModelParamMap.insert(std::make_pair("CDW", std::cref(CDW)));
340  ModelParamMap.insert(std::make_pair("CHWB", std::cref(CHWB)));
341  ModelParamMap.insert(std::make_pair("CHD", std::cref(CHD)));
342  ModelParamMap.insert(std::make_pair("CT", std::cref(CT)));
343  ModelParamMap.insert(std::make_pair("CHbox", std::cref(CHbox)));
344  ModelParamMap.insert(std::make_pair("CH", std::cref(CH)));
345  if (FlagLeptonUniversal) {
346  ModelParamMap.insert(std::make_pair("CHL1", std::cref(CHL1_11)));
347  ModelParamMap.insert(std::make_pair("CHL3", std::cref(CHL3_11)));
348  ModelParamMap.insert(std::make_pair("CHe", std::cref(CHe_11)));
349  ModelParamMap.insert(std::make_pair("CeH_11r", std::cref(CeH_11r)));
350  ModelParamMap.insert(std::make_pair("CeH_22r", std::cref(CeH_22r)));
351  ModelParamMap.insert(std::make_pair("CeH_33r", std::cref(CeH_33r)));
352  ModelParamMap.insert(std::make_pair("CeH_11i", std::cref(CeH_11i)));
353  ModelParamMap.insert(std::make_pair("CeH_22i", std::cref(CeH_22i)));
354  ModelParamMap.insert(std::make_pair("CeH_33i", std::cref(CeH_33i)));
355  ModelParamMap.insert(std::make_pair("CLL", std::cref(CLL_1221)));
356  ModelParamMap.insert(std::make_pair("Cee", std::cref(Cee_1111)));
357  ModelParamMap.insert(std::make_pair("CLe", std::cref(CLe_1111)));
358  } else {
359  ModelParamMap.insert(std::make_pair("CHL1_11", std::cref(CHL1_11)));
360  ModelParamMap.insert(std::make_pair("CHL1_12r", std::cref(CHL1_12r)));
361  ModelParamMap.insert(std::make_pair("CHL1_13r", std::cref(CHL1_13r)));
362  ModelParamMap.insert(std::make_pair("CHL1_22", std::cref(CHL1_22)));
363  ModelParamMap.insert(std::make_pair("CHL1_23r", std::cref(CHL1_23r)));
364  ModelParamMap.insert(std::make_pair("CHL1_33", std::cref(CHL1_33)));
365  ModelParamMap.insert(std::make_pair("CHL1_12i", std::cref(CHL1_12i)));
366  ModelParamMap.insert(std::make_pair("CHL1_13i", std::cref(CHL1_13i)));
367  ModelParamMap.insert(std::make_pair("CHL1_23i", std::cref(CHL1_23i)));
368  ModelParamMap.insert(std::make_pair("CHL3_11", std::cref(CHL3_11)));
369  ModelParamMap.insert(std::make_pair("CHL3_12r", std::cref(CHL3_12r)));
370  ModelParamMap.insert(std::make_pair("CHL3_13r", std::cref(CHL3_13r)));
371  ModelParamMap.insert(std::make_pair("CHL3_22", std::cref(CHL3_22)));
372  ModelParamMap.insert(std::make_pair("CHL3_23r", std::cref(CHL3_23r)));
373  ModelParamMap.insert(std::make_pair("CHL3_33", std::cref(CHL3_33)));
374  ModelParamMap.insert(std::make_pair("CHL3_12i", std::cref(CHL3_12i)));
375  ModelParamMap.insert(std::make_pair("CHL3_13i", std::cref(CHL3_13i)));
376  ModelParamMap.insert(std::make_pair("CHL3_23i", std::cref(CHL3_23i)));
377  ModelParamMap.insert(std::make_pair("CHe_11", std::cref(CHe_11)));
378  ModelParamMap.insert(std::make_pair("CHe_12r", std::cref(CHe_12r)));
379  ModelParamMap.insert(std::make_pair("CHe_13r", std::cref(CHe_13r)));
380  ModelParamMap.insert(std::make_pair("CHe_22", std::cref(CHe_22)));
381  ModelParamMap.insert(std::make_pair("CHe_23r", std::cref(CHe_23r)));
382  ModelParamMap.insert(std::make_pair("CHe_33", std::cref(CHe_33)));
383  ModelParamMap.insert(std::make_pair("CHe_12i", std::cref(CHe_12i)));
384  ModelParamMap.insert(std::make_pair("CHe_13i", std::cref(CHe_13i)));
385  ModelParamMap.insert(std::make_pair("CHe_23i", std::cref(CHe_23i)));
386  ModelParamMap.insert(std::make_pair("CeH_11r", std::cref(CeH_11r)));
387  ModelParamMap.insert(std::make_pair("CeH_12r", std::cref(CeH_12r)));
388  ModelParamMap.insert(std::make_pair("CeH_13r", std::cref(CeH_13r)));
389  ModelParamMap.insert(std::make_pair("CeH_22r", std::cref(CeH_22r)));
390  ModelParamMap.insert(std::make_pair("CeH_23r", std::cref(CeH_23r)));
391  ModelParamMap.insert(std::make_pair("CeH_33r", std::cref(CeH_33r)));
392  ModelParamMap.insert(std::make_pair("CeH_11i", std::cref(CeH_11i)));
393  ModelParamMap.insert(std::make_pair("CeH_12i", std::cref(CeH_12i)));
394  ModelParamMap.insert(std::make_pair("CeH_13i", std::cref(CeH_13i)));
395  ModelParamMap.insert(std::make_pair("CeH_22i", std::cref(CeH_22i)));
396  ModelParamMap.insert(std::make_pair("CeH_23i", std::cref(CeH_23i)));
397  ModelParamMap.insert(std::make_pair("CeH_33i", std::cref(CeH_33i)));
398  ModelParamMap.insert(std::make_pair("CLL_1111", std::cref(CLL_1111)));
399  ModelParamMap.insert(std::make_pair("CLL_1221", std::cref(CLL_1221)));
400  ModelParamMap.insert(std::make_pair("CLL_1122", std::cref(CLL_1122)));
401  ModelParamMap.insert(std::make_pair("CLL_1331", std::cref(CLL_1331)));
402  ModelParamMap.insert(std::make_pair("CLL_1133", std::cref(CLL_1133)));
403  ModelParamMap.insert(std::make_pair("Cee_1111", std::cref(Cee_1111)));
404  ModelParamMap.insert(std::make_pair("Cee_1122", std::cref(Cee_1122)));
405  ModelParamMap.insert(std::make_pair("Cee_1133", std::cref(Cee_1133)));
406  ModelParamMap.insert(std::make_pair("CLe_1111", std::cref(CLe_1111)));
407  ModelParamMap.insert(std::make_pair("CLe_1122", std::cref(CLe_1122)));
408  ModelParamMap.insert(std::make_pair("CLe_2211", std::cref(CLe_2211)));
409  ModelParamMap.insert(std::make_pair("CLe_1133", std::cref(CLe_1133)));
410  ModelParamMap.insert(std::make_pair("CLe_3311", std::cref(CLe_3311)));
411  }
412  if (FlagQuarkUniversal) {
413  ModelParamMap.insert(std::make_pair("CHQ1", std::cref(CHQ1_11)));
414  ModelParamMap.insert(std::make_pair("CHQ3", std::cref(CHQ3_11)));
415  ModelParamMap.insert(std::make_pair("CHu", std::cref(CHu_11)));
416  ModelParamMap.insert(std::make_pair("CHd", std::cref(CHd_11)));
417  ModelParamMap.insert(std::make_pair("CHud_r", std::cref(CHud_11r)));
418  ModelParamMap.insert(std::make_pair("CHud_i", std::cref(CHud_11i)));
419  ModelParamMap.insert(std::make_pair("CuH_11r", std::cref(CuH_11r)));
420  ModelParamMap.insert(std::make_pair("CuH_22r", std::cref(CuH_22r)));
421  ModelParamMap.insert(std::make_pair("CuH_33r", std::cref(CuH_33r)));
422  ModelParamMap.insert(std::make_pair("CuH_11i", std::cref(CuH_11i)));
423  ModelParamMap.insert(std::make_pair("CuH_22i", std::cref(CuH_22i)));
424  ModelParamMap.insert(std::make_pair("CuH_33i", std::cref(CuH_33i)));
425  ModelParamMap.insert(std::make_pair("CdH_11r", std::cref(CdH_11r)));
426  ModelParamMap.insert(std::make_pair("CdH_22r", std::cref(CdH_22r)));
427  ModelParamMap.insert(std::make_pair("CdH_33r", std::cref(CdH_33r)));
428  ModelParamMap.insert(std::make_pair("CdH_11i", std::cref(CdH_11i)));
429  ModelParamMap.insert(std::make_pair("CdH_22i", std::cref(CdH_22i)));
430  ModelParamMap.insert(std::make_pair("CdH_33i", std::cref(CdH_33i)));
431  ModelParamMap.insert(std::make_pair("CuG_r", std::cref(CuG_11r)));
432  ModelParamMap.insert(std::make_pair("CuG_i", std::cref(CuG_11i)));
433  ModelParamMap.insert(std::make_pair("CuW_r", std::cref(CuW_11r)));
434  ModelParamMap.insert(std::make_pair("CuW_i", std::cref(CuW_11i)));
435  ModelParamMap.insert(std::make_pair("CuB_r", std::cref(CuB_11r)));
436  ModelParamMap.insert(std::make_pair("CuB_i", std::cref(CuB_11i)));
437  ModelParamMap.insert(std::make_pair("CdG_r", std::cref(CdG_11r)));
438  ModelParamMap.insert(std::make_pair("CdG_i", std::cref(CdG_11i)));
439  ModelParamMap.insert(std::make_pair("CdW_r", std::cref(CdW_11r)));
440  ModelParamMap.insert(std::make_pair("CdW_i", std::cref(CdW_11i)));
441  ModelParamMap.insert(std::make_pair("CdB_r", std::cref(CdB_11r)));
442  ModelParamMap.insert(std::make_pair("CdB_i", std::cref(CdB_11i)));
443  ModelParamMap.insert(std::make_pair("CeW_r", std::cref(CeW_11r)));
444  ModelParamMap.insert(std::make_pair("CeW_i", std::cref(CeW_11i)));
445  ModelParamMap.insert(std::make_pair("CeB_r", std::cref(CeB_11r)));
446  ModelParamMap.insert(std::make_pair("CeB_i", std::cref(CeB_11i)));
447  } else {
448  ModelParamMap.insert(std::make_pair("CHQ1_11", std::cref(CHQ1_11)));
449  ModelParamMap.insert(std::make_pair("CHQ1_12r", std::cref(CHQ1_12r)));
450  ModelParamMap.insert(std::make_pair("CHQ1_13r", std::cref(CHQ1_13r)));
451  ModelParamMap.insert(std::make_pair("CHQ1_22", std::cref(CHQ1_22)));
452  ModelParamMap.insert(std::make_pair("CHQ1_23r", std::cref(CHQ1_23r)));
453  ModelParamMap.insert(std::make_pair("CHQ1_33", std::cref(CHQ1_33)));
454  ModelParamMap.insert(std::make_pair("CHQ1_12i", std::cref(CHQ1_12i)));
455  ModelParamMap.insert(std::make_pair("CHQ1_13i", std::cref(CHQ1_13i)));
456  ModelParamMap.insert(std::make_pair("CHQ1_23i", std::cref(CHQ1_23i)));
457  ModelParamMap.insert(std::make_pair("CHQ3_11", std::cref(CHQ3_11)));
458  ModelParamMap.insert(std::make_pair("CHQ3_12r", std::cref(CHQ3_12r)));
459  ModelParamMap.insert(std::make_pair("CHQ3_13r", std::cref(CHQ3_13r)));
460  ModelParamMap.insert(std::make_pair("CHQ3_22", std::cref(CHQ3_22)));
461  ModelParamMap.insert(std::make_pair("CHQ3_23r", std::cref(CHQ3_23r)));
462  ModelParamMap.insert(std::make_pair("CHQ3_33", std::cref(CHQ3_33)));
463  ModelParamMap.insert(std::make_pair("CHQ3_12i", std::cref(CHQ3_12i)));
464  ModelParamMap.insert(std::make_pair("CHQ3_13i", std::cref(CHQ3_13i)));
465  ModelParamMap.insert(std::make_pair("CHQ3_23i", std::cref(CHQ3_23i)));
466  ModelParamMap.insert(std::make_pair("CHu_11", std::cref(CHu_11)));
467  ModelParamMap.insert(std::make_pair("CHu_12r", std::cref(CHu_12r)));
468  ModelParamMap.insert(std::make_pair("CHu_13r", std::cref(CHu_13r)));
469  ModelParamMap.insert(std::make_pair("CHu_22", std::cref(CHu_22)));
470  ModelParamMap.insert(std::make_pair("CHu_23r", std::cref(CHu_23r)));
471  ModelParamMap.insert(std::make_pair("CHu_33", std::cref(CHu_33)));
472  ModelParamMap.insert(std::make_pair("CHu_12i", std::cref(CHu_12i)));
473  ModelParamMap.insert(std::make_pair("CHu_13i", std::cref(CHu_13i)));
474  ModelParamMap.insert(std::make_pair("CHu_23i", std::cref(CHu_23i)));
475  ModelParamMap.insert(std::make_pair("CHd_11", std::cref(CHd_11)));
476  ModelParamMap.insert(std::make_pair("CHd_12r", std::cref(CHd_12r)));
477  ModelParamMap.insert(std::make_pair("CHd_13r", std::cref(CHd_13r)));
478  ModelParamMap.insert(std::make_pair("CHd_22", std::cref(CHd_22)));
479  ModelParamMap.insert(std::make_pair("CHd_23r", std::cref(CHd_23r)));
480  ModelParamMap.insert(std::make_pair("CHd_33", std::cref(CHd_33)));
481  ModelParamMap.insert(std::make_pair("CHd_12i", std::cref(CHd_12i)));
482  ModelParamMap.insert(std::make_pair("CHd_13i", std::cref(CHd_13i)));
483  ModelParamMap.insert(std::make_pair("CHd_23i", std::cref(CHd_23i)));
484  ModelParamMap.insert(std::make_pair("CHud_11r", std::cref(CHud_11r)));
485  ModelParamMap.insert(std::make_pair("CHud_12r", std::cref(CHud_12r)));
486  ModelParamMap.insert(std::make_pair("CHud_13r", std::cref(CHud_13r)));
487  ModelParamMap.insert(std::make_pair("CHud_22r", std::cref(CHud_22r)));
488  ModelParamMap.insert(std::make_pair("CHud_23r", std::cref(CHud_23r)));
489  ModelParamMap.insert(std::make_pair("CHud_33r", std::cref(CHud_33r)));
490  ModelParamMap.insert(std::make_pair("CHud_11i", std::cref(CHud_11i)));
491  ModelParamMap.insert(std::make_pair("CHud_12i", std::cref(CHud_12i)));
492  ModelParamMap.insert(std::make_pair("CHud_13i", std::cref(CHud_13i)));
493  ModelParamMap.insert(std::make_pair("CHud_22i", std::cref(CHud_22i)));
494  ModelParamMap.insert(std::make_pair("CHud_23i", std::cref(CHud_23i)));
495  ModelParamMap.insert(std::make_pair("CHud_33i", std::cref(CHud_33i)));
496  ModelParamMap.insert(std::make_pair("CuH_11r", std::cref(CuH_11r)));
497  ModelParamMap.insert(std::make_pair("CuH_12r", std::cref(CuH_12r)));
498  ModelParamMap.insert(std::make_pair("CuH_13r", std::cref(CuH_13r)));
499  ModelParamMap.insert(std::make_pair("CuH_22r", std::cref(CuH_22r)));
500  ModelParamMap.insert(std::make_pair("CuH_23r", std::cref(CuH_23r)));
501  ModelParamMap.insert(std::make_pair("CuH_33r", std::cref(CuH_33r)));
502  ModelParamMap.insert(std::make_pair("CuH_11i", std::cref(CuH_11i)));
503  ModelParamMap.insert(std::make_pair("CuH_12i", std::cref(CuH_12i)));
504  ModelParamMap.insert(std::make_pair("CuH_13i", std::cref(CuH_13i)));
505  ModelParamMap.insert(std::make_pair("CuH_22i", std::cref(CuH_22i)));
506  ModelParamMap.insert(std::make_pair("CuH_23i", std::cref(CuH_23i)));
507  ModelParamMap.insert(std::make_pair("CuH_33i", std::cref(CuH_33i)));
508  ModelParamMap.insert(std::make_pair("CdH_11r", std::cref(CdH_11r)));
509  ModelParamMap.insert(std::make_pair("CdH_12r", std::cref(CdH_12r)));
510  ModelParamMap.insert(std::make_pair("CdH_13r", std::cref(CdH_13r)));
511  ModelParamMap.insert(std::make_pair("CdH_22r", std::cref(CdH_22r)));
512  ModelParamMap.insert(std::make_pair("CdH_23r", std::cref(CdH_23r)));
513  ModelParamMap.insert(std::make_pair("CdH_33r", std::cref(CdH_33r)));
514  ModelParamMap.insert(std::make_pair("CdH_11i", std::cref(CdH_11i)));
515  ModelParamMap.insert(std::make_pair("CdH_12i", std::cref(CdH_12i)));
516  ModelParamMap.insert(std::make_pair("CdH_13i", std::cref(CdH_13i)));
517  ModelParamMap.insert(std::make_pair("CdH_22i", std::cref(CdH_22i)));
518  ModelParamMap.insert(std::make_pair("CdH_23i", std::cref(CdH_23i)));
519  ModelParamMap.insert(std::make_pair("CdH_33i", std::cref(CdH_33i)));
520  ModelParamMap.insert(std::make_pair("CuG_11r", std::cref(CuG_11r)));
521  ModelParamMap.insert(std::make_pair("CuG_12r", std::cref(CuG_12r)));
522  ModelParamMap.insert(std::make_pair("CuG_13r", std::cref(CuG_13r)));
523  ModelParamMap.insert(std::make_pair("CuG_22r", std::cref(CuG_22r)));
524  ModelParamMap.insert(std::make_pair("CuG_23r", std::cref(CuG_23r)));
525  ModelParamMap.insert(std::make_pair("CuG_33r", std::cref(CuG_33r)));
526  ModelParamMap.insert(std::make_pair("CuG_11i", std::cref(CuG_11i)));
527  ModelParamMap.insert(std::make_pair("CuG_12i", std::cref(CuG_12i)));
528  ModelParamMap.insert(std::make_pair("CuG_13i", std::cref(CuG_13i)));
529  ModelParamMap.insert(std::make_pair("CuG_22i", std::cref(CuG_22i)));
530  ModelParamMap.insert(std::make_pair("CuG_23i", std::cref(CuG_23i)));
531  ModelParamMap.insert(std::make_pair("CuG_33i", std::cref(CuG_33i)));
532  ModelParamMap.insert(std::make_pair("CuW_11r", std::cref(CuW_11r)));
533  ModelParamMap.insert(std::make_pair("CuW_12r", std::cref(CuW_12r)));
534  ModelParamMap.insert(std::make_pair("CuW_13r", std::cref(CuW_13r)));
535  ModelParamMap.insert(std::make_pair("CuW_22r", std::cref(CuW_22r)));
536  ModelParamMap.insert(std::make_pair("CuW_23r", std::cref(CuW_23r)));
537  ModelParamMap.insert(std::make_pair("CuW_33r", std::cref(CuW_33r)));
538  ModelParamMap.insert(std::make_pair("CuW_11i", std::cref(CuW_11i)));
539  ModelParamMap.insert(std::make_pair("CuW_12i", std::cref(CuW_12i)));
540  ModelParamMap.insert(std::make_pair("CuW_13i", std::cref(CuW_13i)));
541  ModelParamMap.insert(std::make_pair("CuW_22i", std::cref(CuW_22i)));
542  ModelParamMap.insert(std::make_pair("CuW_23i", std::cref(CuW_23i)));
543  ModelParamMap.insert(std::make_pair("CuW_33i", std::cref(CuW_33i)));
544  ModelParamMap.insert(std::make_pair("CuB_11r", std::cref(CuB_11r)));
545  ModelParamMap.insert(std::make_pair("CuB_12r", std::cref(CuB_12r)));
546  ModelParamMap.insert(std::make_pair("CuB_13r", std::cref(CuB_13r)));
547  ModelParamMap.insert(std::make_pair("CuB_22r", std::cref(CuB_22r)));
548  ModelParamMap.insert(std::make_pair("CuB_23r", std::cref(CuB_23r)));
549  ModelParamMap.insert(std::make_pair("CuB_33r", std::cref(CuB_33r)));
550  ModelParamMap.insert(std::make_pair("CuB_11i", std::cref(CuB_11i)));
551  ModelParamMap.insert(std::make_pair("CuB_12i", std::cref(CuB_12i)));
552  ModelParamMap.insert(std::make_pair("CuB_13i", std::cref(CuB_13i)));
553  ModelParamMap.insert(std::make_pair("CuB_22i", std::cref(CuB_22i)));
554  ModelParamMap.insert(std::make_pair("CuB_23i", std::cref(CuB_23i)));
555  ModelParamMap.insert(std::make_pair("CuB_33i", std::cref(CuB_33i)));
556  ModelParamMap.insert(std::make_pair("CdG_11r", std::cref(CdG_11r)));
557  ModelParamMap.insert(std::make_pair("CdG_12r", std::cref(CdG_12r)));
558  ModelParamMap.insert(std::make_pair("CdG_13r", std::cref(CdG_13r)));
559  ModelParamMap.insert(std::make_pair("CdG_22r", std::cref(CdG_22r)));
560  ModelParamMap.insert(std::make_pair("CdG_23r", std::cref(CdG_23r)));
561  ModelParamMap.insert(std::make_pair("CdG_33r", std::cref(CdG_33r)));
562  ModelParamMap.insert(std::make_pair("CdG_11i", std::cref(CdG_11i)));
563  ModelParamMap.insert(std::make_pair("CdG_12i", std::cref(CdG_12i)));
564  ModelParamMap.insert(std::make_pair("CdG_13i", std::cref(CdG_13i)));
565  ModelParamMap.insert(std::make_pair("CdG_22i", std::cref(CdG_22i)));
566  ModelParamMap.insert(std::make_pair("CdG_23i", std::cref(CdG_23i)));
567  ModelParamMap.insert(std::make_pair("CdG_33i", std::cref(CdG_33i)));
568  ModelParamMap.insert(std::make_pair("CdW_11r", std::cref(CdW_11r)));
569  ModelParamMap.insert(std::make_pair("CdW_12r", std::cref(CdW_12r)));
570  ModelParamMap.insert(std::make_pair("CdW_13r", std::cref(CdW_13r)));
571  ModelParamMap.insert(std::make_pair("CdW_22r", std::cref(CdW_22r)));
572  ModelParamMap.insert(std::make_pair("CdW_23r", std::cref(CdW_23r)));
573  ModelParamMap.insert(std::make_pair("CdW_33r", std::cref(CdW_33r)));
574  ModelParamMap.insert(std::make_pair("CdW_11i", std::cref(CdW_11i)));
575  ModelParamMap.insert(std::make_pair("CdW_12i", std::cref(CdW_12i)));
576  ModelParamMap.insert(std::make_pair("CdW_13i", std::cref(CdW_13i)));
577  ModelParamMap.insert(std::make_pair("CdW_22i", std::cref(CdW_22i)));
578  ModelParamMap.insert(std::make_pair("CdW_23i", std::cref(CdW_23i)));
579  ModelParamMap.insert(std::make_pair("CdW_33i", std::cref(CdW_33i)));
580  ModelParamMap.insert(std::make_pair("CdB_11r", std::cref(CdB_11r)));
581  ModelParamMap.insert(std::make_pair("CdB_12r", std::cref(CdB_12r)));
582  ModelParamMap.insert(std::make_pair("CdB_13r", std::cref(CdB_13r)));
583  ModelParamMap.insert(std::make_pair("CdB_22r", std::cref(CdB_22r)));
584  ModelParamMap.insert(std::make_pair("CdB_23r", std::cref(CdB_23r)));
585  ModelParamMap.insert(std::make_pair("CdB_33r", std::cref(CdB_33r)));
586  ModelParamMap.insert(std::make_pair("CdB_11i", std::cref(CdB_11i)));
587  ModelParamMap.insert(std::make_pair("CdB_12i", std::cref(CdB_12i)));
588  ModelParamMap.insert(std::make_pair("CdB_13i", std::cref(CdB_13i)));
589  ModelParamMap.insert(std::make_pair("CdB_22i", std::cref(CdB_22i)));
590  ModelParamMap.insert(std::make_pair("CdB_23i", std::cref(CdB_23i)));
591  ModelParamMap.insert(std::make_pair("CdB_33i", std::cref(CdB_33i)));
592  ModelParamMap.insert(std::make_pair("CeW_11r", std::cref(CeW_11r)));
593  ModelParamMap.insert(std::make_pair("CeW_12r", std::cref(CeW_12r)));
594  ModelParamMap.insert(std::make_pair("CeW_13r", std::cref(CeW_13r)));
595  ModelParamMap.insert(std::make_pair("CeW_22r", std::cref(CeW_22r)));
596  ModelParamMap.insert(std::make_pair("CeW_23r", std::cref(CeW_23r)));
597  ModelParamMap.insert(std::make_pair("CeW_33r", std::cref(CeW_33r)));
598  ModelParamMap.insert(std::make_pair("CeW_11i", std::cref(CeW_11i)));
599  ModelParamMap.insert(std::make_pair("CeW_12i", std::cref(CeW_12i)));
600  ModelParamMap.insert(std::make_pair("CeW_13i", std::cref(CeW_13i)));
601  ModelParamMap.insert(std::make_pair("CeW_22i", std::cref(CeW_22i)));
602  ModelParamMap.insert(std::make_pair("CeW_23i", std::cref(CeW_23i)));
603  ModelParamMap.insert(std::make_pair("CeW_33i", std::cref(CeW_33i)));
604  ModelParamMap.insert(std::make_pair("CeB_11r", std::cref(CeB_11r)));
605  ModelParamMap.insert(std::make_pair("CeB_12r", std::cref(CeB_12r)));
606  ModelParamMap.insert(std::make_pair("CeB_13r", std::cref(CeB_13r)));
607  ModelParamMap.insert(std::make_pair("CeB_22r", std::cref(CeB_22r)));
608  ModelParamMap.insert(std::make_pair("CeB_23r", std::cref(CeB_23r)));
609  ModelParamMap.insert(std::make_pair("CeB_33r", std::cref(CeB_33r)));
610  ModelParamMap.insert(std::make_pair("CeB_11i", std::cref(CeB_11i)));
611  ModelParamMap.insert(std::make_pair("CeB_12i", std::cref(CeB_12i)));
612  ModelParamMap.insert(std::make_pair("CeB_13i", std::cref(CeB_13i)));
613  ModelParamMap.insert(std::make_pair("CeB_22i", std::cref(CeB_22i)));
614  ModelParamMap.insert(std::make_pair("CeB_23i", std::cref(CeB_23i)));
615  ModelParamMap.insert(std::make_pair("CeB_33i", std::cref(CeB_33i)));
616  }
618  ModelParamMap.insert(std::make_pair("CLQ1", std::cref(CLQ1_1111)));
619  ModelParamMap.insert(std::make_pair("CLQ3", std::cref(CLQ3_1111)));
620  ModelParamMap.insert(std::make_pair("Ceu", std::cref(Ceu_1111)));
621  ModelParamMap.insert(std::make_pair("Ced", std::cref(Ced_1111)));
622  ModelParamMap.insert(std::make_pair("CLu", std::cref(CLu_1111)));
623  ModelParamMap.insert(std::make_pair("CLd", std::cref(CLd_1111)));
624  ModelParamMap.insert(std::make_pair("CQe", std::cref(CQe_1111)));
625  } else {
626  ModelParamMap.insert(std::make_pair("CLQ1_1111", std::cref(CLQ1_1111)));
627  ModelParamMap.insert(std::make_pair("CLQ1_1122", std::cref(CLQ1_1122)));
628  ModelParamMap.insert(std::make_pair("CLQ1_2211", std::cref(CLQ1_2211)));
629  ModelParamMap.insert(std::make_pair("CLQ1_1221", std::cref(CLQ1_1221)));
630  ModelParamMap.insert(std::make_pair("CLQ1_2112", std::cref(CLQ1_2112)));
631  ModelParamMap.insert(std::make_pair("CLQ1_1133", std::cref(CLQ1_1133)));
632  ModelParamMap.insert(std::make_pair("CLQ1_3311", std::cref(CLQ1_3311)));
633  ModelParamMap.insert(std::make_pair("CLQ1_1331", std::cref(CLQ1_1331)));
634  ModelParamMap.insert(std::make_pair("CLQ1_3113", std::cref(CLQ1_3113)));
635  ModelParamMap.insert(std::make_pair("CLQ1_1123", std::cref(CLQ1_1123)));
636  ModelParamMap.insert(std::make_pair("CLQ1_2223", std::cref(CLQ1_2223)));
637  ModelParamMap.insert(std::make_pair("CLQ1_3323", std::cref(CLQ1_3323)));
638  ModelParamMap.insert(std::make_pair("CLQ1_1132", std::cref(CLQ1_1132)));
639  ModelParamMap.insert(std::make_pair("CLQ1_2232", std::cref(CLQ1_2232)));
640  ModelParamMap.insert(std::make_pair("CLQ1_3332", std::cref(CLQ1_3332)));
641  ModelParamMap.insert(std::make_pair("CLQ3_1111", std::cref(CLQ3_1111)));
642  ModelParamMap.insert(std::make_pair("CLQ3_1122", std::cref(CLQ3_1122)));
643  ModelParamMap.insert(std::make_pair("CLQ3_2211", std::cref(CLQ3_2211)));
644  ModelParamMap.insert(std::make_pair("CLQ3_1221", std::cref(CLQ3_1221)));
645  ModelParamMap.insert(std::make_pair("CLQ3_2112", std::cref(CLQ3_2112)));
646  ModelParamMap.insert(std::make_pair("CLQ3_1133", std::cref(CLQ3_1133)));
647  ModelParamMap.insert(std::make_pair("CLQ3_3311", std::cref(CLQ3_3311)));
648  ModelParamMap.insert(std::make_pair("CLQ3_1331", std::cref(CLQ3_1331)));
649  ModelParamMap.insert(std::make_pair("CLQ3_3113", std::cref(CLQ3_3113)));
650  ModelParamMap.insert(std::make_pair("CLQ3_1123", std::cref(CLQ3_1123)));
651  ModelParamMap.insert(std::make_pair("CLQ3_2223", std::cref(CLQ3_2223)));
652  ModelParamMap.insert(std::make_pair("CLQ3_3323", std::cref(CLQ3_3323)));
653  ModelParamMap.insert(std::make_pair("CLQ3_1132", std::cref(CLQ3_1132)));
654  ModelParamMap.insert(std::make_pair("CLQ3_2232", std::cref(CLQ3_2232)));
655  ModelParamMap.insert(std::make_pair("CLQ3_3332", std::cref(CLQ3_3332)));
656  ModelParamMap.insert(std::make_pair("Ceu_1111", std::cref(Ceu_1111)));
657  ModelParamMap.insert(std::make_pair("Ceu_1122", std::cref(Ceu_1122)));
658  ModelParamMap.insert(std::make_pair("Ceu_2211", std::cref(Ceu_2211)));
659  ModelParamMap.insert(std::make_pair("Ceu_1133", std::cref(Ceu_1133)));
660  ModelParamMap.insert(std::make_pair("Ceu_2233", std::cref(Ceu_2233)));
661  ModelParamMap.insert(std::make_pair("Ceu_3311", std::cref(Ceu_3311)));
662  ModelParamMap.insert(std::make_pair("Ced_1111", std::cref(Ced_1111)));
663  ModelParamMap.insert(std::make_pair("Ced_1122", std::cref(Ced_1122)));
664  ModelParamMap.insert(std::make_pair("Ced_2211", std::cref(Ced_2211)));
665  ModelParamMap.insert(std::make_pair("Ced_1133", std::cref(Ced_1133)));
666  ModelParamMap.insert(std::make_pair("Ced_3311", std::cref(Ced_3311)));
667  ModelParamMap.insert(std::make_pair("Ced_1123", std::cref(Ced_1123)));
668  ModelParamMap.insert(std::make_pair("Ced_2223", std::cref(Ced_2223)));
669  ModelParamMap.insert(std::make_pair("Ced_3323", std::cref(Ced_3323)));
670  ModelParamMap.insert(std::make_pair("Ced_1132", std::cref(Ced_1132)));
671  ModelParamMap.insert(std::make_pair("Ced_2232", std::cref(Ced_2232)));
672  ModelParamMap.insert(std::make_pair("Ced_3332", std::cref(Ced_3332)));
673  ModelParamMap.insert(std::make_pair("CLu_1111", std::cref(CLu_1111)));
674  ModelParamMap.insert(std::make_pair("CLu_1122", std::cref(CLu_1122)));
675  ModelParamMap.insert(std::make_pair("CLu_2211", std::cref(CLu_2211)));
676  ModelParamMap.insert(std::make_pair("CLu_1133", std::cref(CLu_1133)));
677  ModelParamMap.insert(std::make_pair("CLu_2233", std::cref(CLu_2233)));
678  ModelParamMap.insert(std::make_pair("CLu_3311", std::cref(CLu_3311)));
679  ModelParamMap.insert(std::make_pair("CLd_1111", std::cref(CLd_1111)));
680  ModelParamMap.insert(std::make_pair("CLd_1122", std::cref(CLd_1122)));
681  ModelParamMap.insert(std::make_pair("CLd_2211", std::cref(CLd_2211)));
682  ModelParamMap.insert(std::make_pair("CLd_1133", std::cref(CLd_1133)));
683  ModelParamMap.insert(std::make_pair("CLd_3311", std::cref(CLd_3311)));
684  ModelParamMap.insert(std::make_pair("CLd_1123", std::cref(CLd_1123)));
685  ModelParamMap.insert(std::make_pair("CLd_2223", std::cref(CLd_2223)));
686  ModelParamMap.insert(std::make_pair("CLd_3323", std::cref(CLd_3323)));
687  ModelParamMap.insert(std::make_pair("CLd_1132", std::cref(CLd_1132)));
688  ModelParamMap.insert(std::make_pair("CLd_2232", std::cref(CLd_2232)));
689  ModelParamMap.insert(std::make_pair("CLd_3332", std::cref(CLd_3332)));
690  ModelParamMap.insert(std::make_pair("CQe_1111", std::cref(CQe_1111)));
691  ModelParamMap.insert(std::make_pair("CQe_1122", std::cref(CQe_1122)));
692  ModelParamMap.insert(std::make_pair("CQe_2211", std::cref(CQe_2211)));
693  ModelParamMap.insert(std::make_pair("CQe_1133", std::cref(CQe_1133)));
694  ModelParamMap.insert(std::make_pair("CQe_3311", std::cref(CQe_3311)));
695  ModelParamMap.insert(std::make_pair("CQe_2311", std::cref(CQe_2311)));
696  ModelParamMap.insert(std::make_pair("CQe_2322", std::cref(CQe_2322)));
697  ModelParamMap.insert(std::make_pair("CQe_2333", std::cref(CQe_2333)));
698  ModelParamMap.insert(std::make_pair("CQe_3211", std::cref(CQe_3211)));
699  ModelParamMap.insert(std::make_pair("CQe_3222", std::cref(CQe_3222)));
700  ModelParamMap.insert(std::make_pair("CQe_3233", std::cref(CQe_3233)));
701  ModelParamMap.insert(std::make_pair("CLedQ_11", std::cref(CLedQ_11)));
702  ModelParamMap.insert(std::make_pair("CLedQ_22", std::cref(CLedQ_22)));
703  ModelParamMap.insert(std::make_pair("CpLedQ_11", std::cref(CpLedQ_11)));
704  ModelParamMap.insert(std::make_pair("CpLedQ_22", std::cref(CpLedQ_22)));
705  }
706  ModelParamMap.insert(std::make_pair("Lambda_NP", std::cref(Lambda_NP)));
707  ModelParamMap.insert(std::make_pair("BrHinv", std::cref(BrHinv)));
708  ModelParamMap.insert(std::make_pair("BrHexo", std::cref(BrHexo)));
709  ModelParamMap.insert(std::make_pair("dg1Z", std::cref(dg1Z)));
710  ModelParamMap.insert(std::make_pair("dKappaga", std::cref(dKappaga)));
711  ModelParamMap.insert(std::make_pair("lambZ", std::cref(lambZ)));
712  ModelParamMap.insert(std::make_pair("eggFint", std::cref(eggFint)));
713  ModelParamMap.insert(std::make_pair("eggFpar", std::cref(eggFpar)));
714  ModelParamMap.insert(std::make_pair("ettHint", std::cref(ettHint)));
715  ModelParamMap.insert(std::make_pair("ettHpar", std::cref(ettHpar)));
716  ModelParamMap.insert(std::make_pair("eVBFint", std::cref(eVBFint)));
717  ModelParamMap.insert(std::make_pair("eVBFpar", std::cref(eVBFpar)));
718  ModelParamMap.insert(std::make_pair("eWHint", std::cref(eWHint)));
719  ModelParamMap.insert(std::make_pair("eWHpar", std::cref(eWHpar)));
720  ModelParamMap.insert(std::make_pair("eZHint", std::cref(eZHint)));
721  ModelParamMap.insert(std::make_pair("eZHpar", std::cref(eZHpar)));
722  ModelParamMap.insert(std::make_pair("eeeWBFint", std::cref(eeeWBFint)));
723  ModelParamMap.insert(std::make_pair("eeeWBFpar", std::cref(eeeWBFpar)));
724  ModelParamMap.insert(std::make_pair("eeeZHint", std::cref(eeeZHint)));
725  ModelParamMap.insert(std::make_pair("eeeZHpar", std::cref(eeeZHpar)));
726  ModelParamMap.insert(std::make_pair("eeettHint", std::cref(eeettHint)));
727  ModelParamMap.insert(std::make_pair("eeettHpar", std::cref(eeettHpar)));
728  ModelParamMap.insert(std::make_pair("eepWBFint", std::cref(eepWBFint)));
729  ModelParamMap.insert(std::make_pair("eepWBFpar", std::cref(eepWBFpar)));
730  ModelParamMap.insert(std::make_pair("eepZBFint", std::cref(eepZBFint)));
731  ModelParamMap.insert(std::make_pair("eepZBFpar", std::cref(eepZBFpar)));
732  ModelParamMap.insert(std::make_pair("eHggint", std::cref(eHggint)));
733  ModelParamMap.insert(std::make_pair("eHggpar", std::cref(eHggpar)));
734  ModelParamMap.insert(std::make_pair("eHWWint", std::cref(eHWWint)));
735  ModelParamMap.insert(std::make_pair("eHWWpar", std::cref(eHWWpar)));
736  ModelParamMap.insert(std::make_pair("eHZZint", std::cref(eHZZint)));
737  ModelParamMap.insert(std::make_pair("eHZZpar", std::cref(eHZZpar)));
738  ModelParamMap.insert(std::make_pair("eHZgaint", std::cref(eHZgaint)));
739  ModelParamMap.insert(std::make_pair("eHZgapar", std::cref(eHZgapar)));
740  ModelParamMap.insert(std::make_pair("eHgagaint", std::cref(eHgagaint)));
741  ModelParamMap.insert(std::make_pair("eHgagapar", std::cref(eHgagapar)));
742  ModelParamMap.insert(std::make_pair("eHmumuint", std::cref(eHmumuint)));
743  ModelParamMap.insert(std::make_pair("eHmumupar", std::cref(eHmumupar)));
744  ModelParamMap.insert(std::make_pair("eHtautauint", std::cref(eHtautauint)));
745  ModelParamMap.insert(std::make_pair("eHtautaupar", std::cref(eHtautaupar)));
746  ModelParamMap.insert(std::make_pair("eHccint", std::cref(eHccint)));
747  ModelParamMap.insert(std::make_pair("eHccpar", std::cref(eHccpar)));
748  ModelParamMap.insert(std::make_pair("eHbbint", std::cref(eHbbint)));
749  ModelParamMap.insert(std::make_pair("eHbbpar", std::cref(eHbbpar)));
750  ModelParamMap.insert(std::make_pair("eggFHgaga", std::cref(eggFHgaga)));
751  ModelParamMap.insert(std::make_pair("eggFHZga", std::cref(eggFHZga)));
752  ModelParamMap.insert(std::make_pair("eggFHZZ", std::cref(eggFHZZ)));
753  ModelParamMap.insert(std::make_pair("eggFHWW", std::cref(eggFHWW)));
754  ModelParamMap.insert(std::make_pair("eggFHtautau", std::cref(eggFHtautau)));
755  ModelParamMap.insert(std::make_pair("eggFHbb", std::cref(eggFHbb)));
756  ModelParamMap.insert(std::make_pair("eggFHmumu", std::cref(eggFHmumu)));
757  ModelParamMap.insert(std::make_pair("eVBFHgaga", std::cref(eVBFHgaga)));
758  ModelParamMap.insert(std::make_pair("eVBFHZga", std::cref(eVBFHZga)));
759  ModelParamMap.insert(std::make_pair("eVBFHZZ", std::cref(eVBFHZZ)));
760  ModelParamMap.insert(std::make_pair("eVBFHWW", std::cref(eVBFHWW)));
761  ModelParamMap.insert(std::make_pair("eVBFHtautau", std::cref(eVBFHtautau)));
762  ModelParamMap.insert(std::make_pair("eVBFHbb", std::cref(eVBFHbb)));
763  ModelParamMap.insert(std::make_pair("eVBFHmumu", std::cref(eVBFHmumu)));
764  ModelParamMap.insert(std::make_pair("eWHgaga", std::cref(eWHgaga)));
765  ModelParamMap.insert(std::make_pair("eWHZga", std::cref(eWHZga)));
766  ModelParamMap.insert(std::make_pair("eWHZZ", std::cref(eWHZZ)));
767  ModelParamMap.insert(std::make_pair("eWHWW", std::cref(eWHWW)));
768  ModelParamMap.insert(std::make_pair("eWHtautau", std::cref(eWHtautau)));
769  ModelParamMap.insert(std::make_pair("eWHbb", std::cref(eWHbb)));
770  ModelParamMap.insert(std::make_pair("eWHmumu", std::cref(eWHmumu)));
771  ModelParamMap.insert(std::make_pair("eZHgaga", std::cref(eZHgaga)));
772  ModelParamMap.insert(std::make_pair("eZHZga", std::cref(eZHZga)));
773  ModelParamMap.insert(std::make_pair("eZHZZ", std::cref(eZHZZ)));
774  ModelParamMap.insert(std::make_pair("eZHWW", std::cref(eZHWW)));
775  ModelParamMap.insert(std::make_pair("eZHtautau", std::cref(eZHtautau)));
776  ModelParamMap.insert(std::make_pair("eZHbb", std::cref(eZHbb)));
777  ModelParamMap.insert(std::make_pair("eZHmumu", std::cref(eZHmumu)));
778  ModelParamMap.insert(std::make_pair("ettHgaga", std::cref(ettHgaga)));
779  ModelParamMap.insert(std::make_pair("ettHZga", std::cref(ettHZga)));
780  ModelParamMap.insert(std::make_pair("ettHZZ", std::cref(ettHZZ)));
781  ModelParamMap.insert(std::make_pair("ettHWW", std::cref(ettHWW)));
782  ModelParamMap.insert(std::make_pair("ettHtautau", std::cref(ettHtautau)));
783  ModelParamMap.insert(std::make_pair("ettHbb", std::cref(ettHbb)));
784  ModelParamMap.insert(std::make_pair("ettHmumu", std::cref(ettHmumu)));
785  ModelParamMap.insert(std::make_pair("eVBFHinv", std::cref(eVBFHinv)));
786  ModelParamMap.insert(std::make_pair("eVHinv", std::cref(eVHinv)));
787  ModelParamMap.insert(std::make_pair("eVBF_2_Hbox", std::cref(eVBF_2_Hbox)));
788  ModelParamMap.insert(std::make_pair("eVBF_2_HQ1_11", std::cref(eVBF_2_HQ1_11)));
789  ModelParamMap.insert(std::make_pair("eVBF_2_Hu_11", std::cref(eVBF_2_Hu_11)));
790  ModelParamMap.insert(std::make_pair("eVBF_2_Hd_11", std::cref(eVBF_2_Hd_11)));
791  ModelParamMap.insert(std::make_pair("eVBF_2_HQ3_11", std::cref(eVBF_2_HQ3_11)));
792  ModelParamMap.insert(std::make_pair("eVBF_2_HD", std::cref(eVBF_2_HD)));
793  ModelParamMap.insert(std::make_pair("eVBF_2_HB", std::cref(eVBF_2_HB)));
794  ModelParamMap.insert(std::make_pair("eVBF_2_HW", std::cref(eVBF_2_HW)));
795  ModelParamMap.insert(std::make_pair("eVBF_2_HWB", std::cref(eVBF_2_HWB)));
796  ModelParamMap.insert(std::make_pair("eVBF_2_HG", std::cref(eVBF_2_HG)));
797  ModelParamMap.insert(std::make_pair("eVBF_2_DHB", std::cref(eVBF_2_DHB)));
798  ModelParamMap.insert(std::make_pair("eVBF_2_DHW", std::cref(eVBF_2_DHW)));
799  ModelParamMap.insert(std::make_pair("eVBF_2_DeltaGF", std::cref(eVBF_2_DeltaGF)));
800  ModelParamMap.insert(std::make_pair("eVBF_78_Hbox", std::cref(eVBF_78_Hbox)));
801  ModelParamMap.insert(std::make_pair("eVBF_78_HQ1_11", std::cref(eVBF_78_HQ1_11)));
802  ModelParamMap.insert(std::make_pair("eVBF_78_Hu_11", std::cref(eVBF_78_Hu_11)));
803  ModelParamMap.insert(std::make_pair("eVBF_78_Hd_11", std::cref(eVBF_78_Hd_11)));
804  ModelParamMap.insert(std::make_pair("eVBF_78_HQ3_11", std::cref(eVBF_78_HQ3_11)));
805  ModelParamMap.insert(std::make_pair("eVBF_78_HD", std::cref(eVBF_78_HD)));
806  ModelParamMap.insert(std::make_pair("eVBF_78_HB", std::cref(eVBF_78_HB)));
807  ModelParamMap.insert(std::make_pair("eVBF_78_HW", std::cref(eVBF_78_HW)));
808  ModelParamMap.insert(std::make_pair("eVBF_78_HWB", std::cref(eVBF_78_HWB)));
809  ModelParamMap.insert(std::make_pair("eVBF_78_HG", std::cref(eVBF_78_HG)));
810  ModelParamMap.insert(std::make_pair("eVBF_78_DHB", std::cref(eVBF_78_DHB)));
811  ModelParamMap.insert(std::make_pair("eVBF_78_DHW", std::cref(eVBF_78_DHW)));
812  ModelParamMap.insert(std::make_pair("eVBF_78_DeltaGF", std::cref(eVBF_78_DeltaGF)));
813  ModelParamMap.insert(std::make_pair("eVBF_1314_Hbox", std::cref(eVBF_1314_Hbox)));
814  ModelParamMap.insert(std::make_pair("eVBF_1314_HQ1_11", std::cref(eVBF_1314_HQ1_11)));
815  ModelParamMap.insert(std::make_pair("eVBF_1314_Hu_11", std::cref(eVBF_1314_Hu_11)));
816  ModelParamMap.insert(std::make_pair("eVBF_1314_Hd_11", std::cref(eVBF_1314_Hd_11)));
817  ModelParamMap.insert(std::make_pair("eVBF_1314_HQ3_11", std::cref(eVBF_1314_HQ3_11)));
818  ModelParamMap.insert(std::make_pair("eVBF_1314_HD", std::cref(eVBF_1314_HD)));
819  ModelParamMap.insert(std::make_pair("eVBF_1314_HB", std::cref(eVBF_1314_HB)));
820  ModelParamMap.insert(std::make_pair("eVBF_1314_HW", std::cref(eVBF_1314_HW)));
821  ModelParamMap.insert(std::make_pair("eVBF_1314_HWB", std::cref(eVBF_1314_HWB)));
822  ModelParamMap.insert(std::make_pair("eVBF_1314_HG", std::cref(eVBF_1314_HG)));
823  ModelParamMap.insert(std::make_pair("eVBF_1314_DHB", std::cref(eVBF_1314_DHB)));
824  ModelParamMap.insert(std::make_pair("eVBF_1314_DHW", std::cref(eVBF_1314_DHW)));
825  ModelParamMap.insert(std::make_pair("eVBF_1314_DeltaGF", std::cref(eVBF_1314_DeltaGF)));
826  ModelParamMap.insert(std::make_pair("eWH_2_Hbox", std::cref(eWH_2_Hbox)));
827  ModelParamMap.insert(std::make_pair("eWH_2_HQ3_11", std::cref(eWH_2_HQ3_11)));
828  ModelParamMap.insert(std::make_pair("eWH_2_HD", std::cref(eWH_2_HD)));
829  ModelParamMap.insert(std::make_pair("eWH_2_HW", std::cref(eWH_2_HW)));
830  ModelParamMap.insert(std::make_pair("eWH_2_HWB", std::cref(eWH_2_HWB)));
831  ModelParamMap.insert(std::make_pair("eWH_2_DHW", std::cref(eWH_2_DHW)));
832  ModelParamMap.insert(std::make_pair("eWH_2_DeltaGF", std::cref(eWH_2_DeltaGF)));
833  ModelParamMap.insert(std::make_pair("eWH_78_Hbox", std::cref(eWH_78_Hbox)));
834  ModelParamMap.insert(std::make_pair("eWH_78_HQ3_11", std::cref(eWH_78_HQ3_11)));
835  ModelParamMap.insert(std::make_pair("eWH_78_HD", std::cref(eWH_78_HD)));
836  ModelParamMap.insert(std::make_pair("eWH_78_HW", std::cref(eWH_78_HW)));
837  ModelParamMap.insert(std::make_pair("eWH_78_HWB", std::cref(eWH_78_HWB)));
838  ModelParamMap.insert(std::make_pair("eWH_78_DHW", std::cref(eWH_78_DHW)));
839  ModelParamMap.insert(std::make_pair("eWH_78_DeltaGF", std::cref(eWH_78_DeltaGF)));
840  ModelParamMap.insert(std::make_pair("eWH_1314_Hbox", std::cref(eWH_1314_Hbox)));
841  ModelParamMap.insert(std::make_pair("eWH_1314_HQ3_11", std::cref(eWH_1314_HQ3_11)));
842  ModelParamMap.insert(std::make_pair("eWH_1314_HD", std::cref(eWH_1314_HD)));
843  ModelParamMap.insert(std::make_pair("eWH_1314_HW", std::cref(eWH_1314_HW)));
844  ModelParamMap.insert(std::make_pair("eWH_1314_HWB", std::cref(eWH_1314_HWB)));
845  ModelParamMap.insert(std::make_pair("eWH_1314_DHW", std::cref(eWH_1314_DHW)));
846  ModelParamMap.insert(std::make_pair("eWH_1314_DeltaGF", std::cref(eWH_1314_DeltaGF)));
847  ModelParamMap.insert(std::make_pair("eZH_2_Hbox", std::cref(eZH_2_Hbox)));
848  ModelParamMap.insert(std::make_pair("eZH_2_HQ1_11", std::cref(eZH_2_HQ1_11)));
849  ModelParamMap.insert(std::make_pair("eZH_2_Hu_11", std::cref(eZH_2_Hu_11)));
850  ModelParamMap.insert(std::make_pair("eZH_2_Hd_11", std::cref(eZH_2_Hd_11)));
851  ModelParamMap.insert(std::make_pair("eZH_2_HQ3_11", std::cref(eZH_2_HQ3_11)));
852  ModelParamMap.insert(std::make_pair("eZH_2_HD", std::cref(eZH_2_HD)));
853  ModelParamMap.insert(std::make_pair("eZH_2_HB", std::cref(eZH_2_HB)));
854  ModelParamMap.insert(std::make_pair("eZH_2_HW", std::cref(eZH_2_HW)));
855  ModelParamMap.insert(std::make_pair("eZH_2_HWB", std::cref(eZH_2_HWB)));
856  ModelParamMap.insert(std::make_pair("eZH_2_DHB", std::cref(eZH_2_DHB)));
857  ModelParamMap.insert(std::make_pair("eZH_2_DHW", std::cref(eZH_2_DHW)));
858  ModelParamMap.insert(std::make_pair("eZH_2_DeltaGF", std::cref(eZH_2_DeltaGF)));
859  ModelParamMap.insert(std::make_pair("eZH_78_Hbox", std::cref(eZH_78_Hbox)));
860  ModelParamMap.insert(std::make_pair("eZH_78_HQ1_11", std::cref(eZH_78_HQ1_11)));
861  ModelParamMap.insert(std::make_pair("eZH_78_Hu_11", std::cref(eZH_78_Hu_11)));
862  ModelParamMap.insert(std::make_pair("eZH_78_Hd_11", std::cref(eZH_78_Hd_11)));
863  ModelParamMap.insert(std::make_pair("eZH_78_HQ3_11", std::cref(eZH_78_HQ3_11)));
864  ModelParamMap.insert(std::make_pair("eZH_78_HD", std::cref(eZH_78_HD)));
865  ModelParamMap.insert(std::make_pair("eZH_78_HB", std::cref(eZH_78_HB)));
866  ModelParamMap.insert(std::make_pair("eZH_78_HW", std::cref(eZH_78_HW)));
867  ModelParamMap.insert(std::make_pair("eZH_78_HWB", std::cref(eZH_78_HWB)));
868  ModelParamMap.insert(std::make_pair("eZH_78_DHB", std::cref(eZH_78_DHB)));
869  ModelParamMap.insert(std::make_pair("eZH_78_DHW", std::cref(eZH_78_DHW)));
870  ModelParamMap.insert(std::make_pair("eZH_78_DeltaGF", std::cref(eZH_78_DeltaGF)));
871  ModelParamMap.insert(std::make_pair("eZH_1314_Hbox", std::cref(eZH_1314_Hbox)));
872  ModelParamMap.insert(std::make_pair("eZH_1314_HQ1_11", std::cref(eZH_1314_HQ1_11)));
873  ModelParamMap.insert(std::make_pair("eZH_1314_Hu_11", std::cref(eZH_1314_Hu_11)));
874  ModelParamMap.insert(std::make_pair("eZH_1314_Hd_11", std::cref(eZH_1314_Hd_11)));
875  ModelParamMap.insert(std::make_pair("eZH_1314_HQ3_11", std::cref(eZH_1314_HQ3_11)));
876  ModelParamMap.insert(std::make_pair("eZH_1314_HD", std::cref(eZH_1314_HD)));
877  ModelParamMap.insert(std::make_pair("eZH_1314_HB", std::cref(eZH_1314_HB)));
878  ModelParamMap.insert(std::make_pair("eZH_1314_HW", std::cref(eZH_1314_HW)));
879  ModelParamMap.insert(std::make_pair("eZH_1314_HWB", std::cref(eZH_1314_HWB)));
880  ModelParamMap.insert(std::make_pair("eZH_1314_DHB", std::cref(eZH_1314_DHB)));
881  ModelParamMap.insert(std::make_pair("eZH_1314_DHW", std::cref(eZH_1314_DHW)));
882  ModelParamMap.insert(std::make_pair("eZH_1314_DeltaGF", std::cref(eZH_1314_DeltaGF)));
883  ModelParamMap.insert(std::make_pair("ettH_2_HG", std::cref(ettH_2_HG)));
884  ModelParamMap.insert(std::make_pair("ettH_2_G", std::cref(ettH_2_G)));
885  ModelParamMap.insert(std::make_pair("ettH_2_uG_33r", std::cref(ettH_2_uG_33r)));
886  ModelParamMap.insert(std::make_pair("ettH_2_DeltagHt", std::cref(ettH_2_DeltagHt)));
887  ModelParamMap.insert(std::make_pair("ettH_78_HG", std::cref(ettH_78_HG)));
888  ModelParamMap.insert(std::make_pair("ettH_78_G", std::cref(ettH_78_G)));
889  ModelParamMap.insert(std::make_pair("ettH_78_uG_33r", std::cref(ettH_78_uG_33r)));
890  ModelParamMap.insert(std::make_pair("ettH_78_DeltagHt", std::cref(ettH_78_DeltagHt)));
891  ModelParamMap.insert(std::make_pair("ettH_1314_HG", std::cref(ettH_1314_HG)));
892  ModelParamMap.insert(std::make_pair("ettH_1314_G", std::cref(ettH_1314_G)));
893  ModelParamMap.insert(std::make_pair("ettH_1314_uG_33r", std::cref(ettH_1314_uG_33r)));
894  ModelParamMap.insert(std::make_pair("ettH_1314_DeltagHt", std::cref(ettH_1314_DeltagHt)));
895 
896  if (FlagLeptonUniversal) {
897  CeH_12r = 0.0;
898  CeH_13r = 0.0;
899  CeH_23r = 0.0;
900  CeH_12i = 0.0;
901  CeH_13i = 0.0;
902  CeH_23i = 0.0;
903 
904 // bsll/sbll entries only interesting (for the moment) if non-lepton universal. Set to 0 otherwise
905  CLQ1_1123 = 0.0;
906  CLQ1_2223 = 0.0;
907  CLQ1_3323 = 0.0;
908  CLQ1_1132 = 0.0;
909  CLQ1_2232 = 0.0;
910  CLQ1_3332 = 0.0;
911 
912  CLQ3_1123 = 0.0;
913  CLQ3_2223 = 0.0;
914  CLQ3_3323 = 0.0;
915  CLQ3_1132 = 0.0;
916  CLQ3_2232 = 0.0;
917  CLQ3_3332 = 0.0;
918 
919  Ced_1123 = 0.0;
920  Ced_2223 = 0.0;
921  Ced_3323 = 0.0;
922  Ced_1132 = 0.0;
923  Ced_2232 = 0.0;
924  Ced_3332 = 0.0;
925 
926  CLd_1123 = 0.0;
927  CLd_2223 = 0.0;
928  CLd_3323 = 0.0;
929  CLd_1132 = 0.0;
930  CLd_2232 = 0.0;
931  CLd_3332 = 0.0;
932 
933  CQe_2311 = 0.0;
934  CQe_2322 = 0.0;
935  CQe_2333 = 0.0;
936  CQe_3211 = 0.0;
937  CQe_3222 = 0.0;
938  CQe_3233 = 0.0;
939  }
940  if (FlagQuarkUniversal) {
941  CuH_12r = 0.0;
942  CuH_13r = 0.0;
943  CuH_23r = 0.0;
944  CuH_12i = 0.0;
945  CuH_13i = 0.0;
946  CuH_23i = 0.0;
947 
948  CdH_12r = 0.0;
949  CdH_13r = 0.0;
950  CdH_23r = 0.0;
951  CdH_12i = 0.0;
952  CdH_13i = 0.0;
953  CdH_23i = 0.0;
954  }
955 }

Member Function Documentation

◆ AH_f()

gslpp::complex NPSMEFTd6::AH_f ( const double  tau) const

Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)

Parameters
[in]

Definition at line 3595 of file NPSMEFTd6.cpp.

3596 {
3597  return (2.0 * tau * (1.0 + (1.0 - tau) * f_triangle(tau)));
3598 }

◆ AH_W()

gslpp::complex NPSMEFTd6::AH_W ( const double  tau) const

W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling.

\(A^H_W(\tau)=-[2+3\tau + 3\tau*(2-\tau) f(\tau)]\)

Parameters
[in]

Definition at line 3600 of file NPSMEFTd6.cpp.

3601 {
3602  return -( 2.0 + 3.0 * tau + 3.0 * tau * (2.0 - tau) * f_triangle(tau) );
3603 }

◆ AHZga_f()

gslpp::complex NPSMEFTd6::AHZga_f ( const double  tau,
const double  lambda 
) const

Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3605 of file NPSMEFTd6.cpp.

3606 {
3607  return I_triangle_1(tau,lambda) - I_triangle_2(tau,lambda);
3608 }

◆ AHZga_W()

gslpp::complex NPSMEFTd6::AHZga_W ( const double  tau,
const double  lambda 
) const

W loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3610 of file NPSMEFTd6.cpp.

3611 {
3612  gslpp::complex tmp;
3613 
3614  double tan2w = trueSM.sW2() / trueSM.cW2();
3615 
3616  tmp = 4.0 * (3.0 - tan2w ) * I_triangle_2(tau,lambda);
3617 
3618  tmp = tmp + ((1.0 +2.0 / tau)* tan2w - (5.0 + 2.0/tau)) * I_triangle_1(tau,lambda);
3619 
3620  return sqrt(trueSM.cW2()) * tmp;
3621 }

◆ aPskPol()

double NPSMEFTd6::aPskPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(a_{eeZH}\)

Reimplemented from NPbase.

Definition at line 8939 of file NPSMEFTd6.cpp.

8940 {
8941 
8942  // Expression missing CLL contributions!
8943 
8944  double aL, aR, aPol;
8945  double sM = sqrt_s * sqrt_s;
8946  double Mz2 = Mz*Mz;
8947  double MH2 = mHl*mHl;
8948  double dMz = 0.0;
8949  double dMH = 0.0;
8950  double dv,dg,dgp,dgL,dgR;
8951  double kCM, kCM2, EZ, EZ2, kZ, kH;
8952  double EtaZ;
8953  double CHpsk, CTpsk,CHL,CHLp, CHE;
8954  double CWB, CBB, CWW;
8955 
8956  // Convention for dim 6 operators
8958  CBB = 0.25 * (g2_tree*g2_tree/g1_tree/g1_tree) * CiHB * v2_over_LambdaNP2;
8959  CWW = 0.25 * CiHW * v2_over_LambdaNP2;
8960 
8961  CHpsk = ( -2.0 * CiHbox + 0.25 * CiHD ) * v2_over_LambdaNP2;
8962  CTpsk = -0.5 * CiHD * v2_over_LambdaNP2;
8963  CHL = CiHL1_11 * v2_over_LambdaNP2;
8964  CHLp = CiHL3_11 * v2_over_LambdaNP2;
8965  CHE = CiHe_11 * v2_over_LambdaNP2;
8966 
8967  // Other parameters (1): Missing CLL!!!
8968  dv = 0.5 * ( CiHL3_11 + CiHL3_22 )* v2_over_LambdaNP2;
8969 
8970  // WFR
8971  EtaZ = -(1.0/2.0)*CHpsk + 2.0*dMz - dv - CTpsk;
8972 
8973  // Kinematics
8974  kCM = sqrt( (sM*sM + (MH2 - Mz2)*(MH2 - Mz2) - 2.0*sM*(MH2 + Mz2))/(4.0*sM) );
8975  kCM2 = kCM*kCM;
8976 
8977  EZ = sqrt( Mz2 + kCM2);
8978  EZ2 = EZ*EZ;
8979 
8980  kZ = 2.0*Mz2/(sM - Mz2) + (EZ*Mz2)/(2*kCM2*sqrt_s) - Mz2/(2*kCM2) - (EZ2/Mz2)/(2.0 + EZ2/Mz2)*(1.0 - Mz2/(EZ*sqrt_s));
8981 
8982  kH = -((EZ*MH2)/(2*kCM2*sqrt_s)) - (EZ2/Mz2)/(2 + EZ2/Mz2)*MH2/(EZ*sqrt_s);
8983 
8984  // Other parameters (2): Missing CLL!!!
8985  dg = -(1.0/(g1_tree * ( cW2_tree*cW2_tree - sW2_tree*sW2_tree))) * ( dv * cW2_tree * g1_tree
8986  - cW2_tree * dMz * g1_tree + 0.25 * CiHD * cW2_tree * g1_tree * v2_over_LambdaNP2
8989 
8990 
8991  dgp = -(1.0/(cW2_tree * g1_tree * g1_tree * (-cW2_tree*cW2_tree + sW2_tree*sW2_tree))) * ( dv * cW2_tree * g1_tree * g1_tree * sW2_tree
8997 
8998  dgL = (1.0/(0.5 - sW2_tree))*(cW2_tree*(0.5 + sW2_tree)*dg
8999  - sW2_tree*(0.5 + cW2_tree)*dgp
9000  + 0.5*(CHL + CHLp)
9001  + 0.25*cW2_tree*(1.0 + 2.0*sW2_tree)*8.0*CWW
9002  - 0.5*sW2_tree*(1.0 - 2.0*sW2_tree)*8.0*CWB
9003  - 0.25*sW2_tree*sW2_tree/cW2_tree*(1.0 + 2.0*cW2_tree)*8.0*CBB);
9004 
9005  dgR = -cW2_tree*dg + (1.0 + cW2_tree)*dgp
9006  - 1.0/(2.0*sW2_tree)*CHE - 0.5*cW2_tree*8*CWW
9007  + cW2_tree*8.0*CWB + 0.5*sW2_tree/cW2_tree*(1.0 + cW2_tree)*8.0*CBB;
9008 
9009 
9010  // LH and RH pars
9011 
9012  aL = dgL + 2*dMz - dv + EtaZ + (sM - Mz2)/(2*Mz2)*(CHL + CHLp)/(0.5 - sW2_tree) + kZ*dMz + kH*dMH;
9013  aR = dgR + 2*dMz - dv + EtaZ - (sM - Mz2)/(2*Mz2)*CHE/sW2_tree + kZ*dMz + kH*dMH;
9014 
9015  // Polarized a parameter
9016  aPol = 0.25 * ( (1.0 - Pol_em/100.0)*(1.0 + Pol_ep/100.0) * aL
9017  + (1.0 + Pol_em/100.0)*(1.0 - Pol_ep/100.0) * aR );
9018 
9019  return aPol;
9020 }

◆ AuxObs_NP1()

double NPSMEFTd6::AuxObs_NP1 ( ) const
virtual

Auxiliary observable AuxObs_NP1 (See code for details.)

Returns
AuxObs_NP1

Reimplemented from NPbase.

Definition at line 15619 of file NPSMEFTd6.cpp.

15620 {
15621  // To be used for some temporary observable
15622 
15623  // WY analysis at 13 TeV for HL-LHC 3/ab
15624  double Wpar, Ypar, Wpar2, Ypar2;
15625  double Chi2NC13, Chi2CC13, Chi2Tot;
15626 
15627  Wpar = 10000.0 * obliqueW();
15628  Ypar = 10000.0 * obliqueY();
15629 
15630  Wpar2 = Wpar*Wpar;
15631  Ypar2 = Ypar*Ypar;
15632 
15633  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
15634 
15635  Chi2NC13 = 0.032772034538390675 * Wpar2*Wpar2 + 2.815243944990361 * Ypar2 - 0.36522061776278516 * Ypar2*Ypar
15636  + 0.017375258924241194 * Ypar2*Ypar2 + Wpar2*Wpar * (-0.7059117582389635 + 0.006816297425306027 * Ypar)
15637  + Wpar * Ypar * (7.988302197022343 + Ypar * (-0.5450119819316416 + 0.0050292149953719766 * Ypar))
15638  + Wpar2 * (5.68581760491364 + Ypar * (-0.5794111075840261 + 0.048026245835369625 * Ypar));
15639 
15640  Chi2Tot = Chi2CC13 + Chi2NC13;
15641 
15642  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15643  return sqrt(Chi2Tot);
15644 }

◆ AuxObs_NP10()

double NPSMEFTd6::AuxObs_NP10 ( ) const
virtual

Auxiliary observable AuxObs_NP10 (See code for details.)

Returns
AuxObs_NP10

Reimplemented from NPbase.

Definition at line 16220 of file NPSMEFTd6.cpp.

16221 {
16222  // CLIC STWY using difermion production at all energies: 380 and 1500 GeV
16223  double Spar, Tpar, Wpar, Ypar, Spar2, Tpar2, Wpar2, Ypar2;
16224  double Chi2Tot;
16225 
16226  Spar = obliqueS();
16227  Tpar = obliqueT();
16228  Wpar = 10000.0 * obliqueW();
16229  Ypar = 10000.0 * obliqueY();
16230 
16231  Spar2 = Spar*Spar;
16232  Tpar2 = Tpar*Tpar;
16233  Wpar2 = Wpar*Wpar;
16234  Ypar2 = Ypar*Ypar;
16235 
16236  Chi2Tot = 375.63808963031073 * Spar2
16237  - 617.8864704052573 * Spar * Tpar
16238  + 353.1650032169891 * Tpar2
16239  + 215.96605851087603 * Spar * Wpar
16240  - 309.3469843690006 * Tpar * Wpar
16241  + 518.10263970583244 * Wpar2
16242  - 45.972763923203014 * Spar * Ypar
16243  - 40.670385844305705 * Tpar * Ypar
16244  + 340.56677318671185 * Wpar * Ypar
16245  + 364.5290176991845 * Ypar2;
16246 
16247  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16248  return sqrt(Chi2Tot);
16249 }

◆ AuxObs_NP11()

double NPSMEFTd6::AuxObs_NP11 ( ) const
virtual

Auxiliary observable AuxObs_NP11 (See code for details.)

Returns
AuxObs_NP11

Reimplemented from NPbase.

Definition at line 16251 of file NPSMEFTd6.cpp.

16252 {
16253  // CLIC STWY using difermion production at all energies: 380 GeV
16254  double Spar, Tpar, Wpar, Ypar, Spar2, Tpar2, Wpar2, Ypar2;
16255  double Chi2Tot;
16256 
16257  Spar = obliqueS();
16258  Tpar = obliqueT();
16259  Wpar = 10000.0 * obliqueW();
16260  Ypar = 10000.0 * obliqueY();
16261 
16262  Spar2 = Spar*Spar;
16263  Tpar2 = Tpar*Tpar;
16264  Wpar2 = Wpar*Wpar;
16265  Ypar2 = Ypar*Ypar;
16266 
16267  Chi2Tot = 282.9842573293628 * Spar2
16268  - 462.32090035841725 * Spar * Tpar
16269  + 276.2496928300019 * Tpar2
16270  + 66.08702076419566 * Spar * Wpar
16271  - 87.95794393624075 * Tpar * Wpar
16272  + 9.5435699879102 * Wpar2
16273  - 26.170009941328716 * Spar * Ypar
16274  - 9.695238064023518 * Tpar * Ypar
16275  + 6.519573295893438 * Wpar * Ypar
16276  + 12.858593910798793 * Ypar2;
16277 
16278  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16279  return sqrt(Chi2Tot);
16280 }

◆ AuxObs_NP12()

double NPSMEFTd6::AuxObs_NP12 ( ) const
virtual

Auxiliary observable AuxObs_NP12 (See code for details.)

Returns
AuxObs_NP12

Reimplemented from NPbase.

Definition at line 16282 of file NPSMEFTd6.cpp.

16283 {
16284  // CLIC dim6 Top fit 1500 GeV: only for SVF operators
16285  double CHqminus, CHt;
16286  double Chi2Tot;
16287 
16288  // The chi2 is given assuming C/Lambda^2 is in units of TeV^-2
16289  CHqminus= 0.5 * (CiHQ1_33 - CiHQ3_33) * (1000000.0 / LambdaNP2);
16290  CHt= 0.5 * CiHu_33 * (1000000.0 / LambdaNP2);
16291 
16292  Chi2Tot= 1203.58 * CHqminus * CHqminus + 1661.59 * CHqminus * CHt + 1257.83 * CHt * CHt;
16293 
16294  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16295  return sqrt(Chi2Tot);
16296 }

◆ AuxObs_NP13()

double NPSMEFTd6::AuxObs_NP13 ( ) const
virtual

Auxiliary observable AuxObs_NP13.

Returns
AuxObs_NP13

Reimplemented from NPbase.

Definition at line 16298 of file NPSMEFTd6.cpp.

16299 {
16300  // CLIC dim6 Top fit 3000 GeV: only for SVF operators
16301  double CHqminus, CHt;
16302  double Chi2Tot;
16303 
16304  // The chi2 is given assuming C/Lambda^2 is in units of TeV^-2
16305  CHqminus= 0.5 * (CiHQ1_33 - CiHQ3_33) * (1000000.0 / LambdaNP2);
16306  CHt= 0.5 * CiHu_33 * (1000000.0 / LambdaNP2);
16307 
16308  Chi2Tot= 5756.01 * CHqminus * CHqminus + 8013.79 * CHqminus * CHt + 3380.7 * CHt * CHt;
16309 
16310  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16311  return sqrt(Chi2Tot);
16312 }

◆ AuxObs_NP14()

double NPSMEFTd6::AuxObs_NP14 ( ) const
virtual

Auxiliary observable AuxObs_NP14.

Returns
AuxObs_NP14

Reimplemented from NPbase.

Definition at line 16314 of file NPSMEFTd6.cpp.

16315 {
16316  // Test chi2 for HH production at 100 TeV: only the first two bins in 1704.01953 are included,
16317  // with the same coefficients (including ratios of cross sections in each bin) its table 4. The EFT parameterization of Higgs decays are not included.
16318  double Chi2Tot;
16319 
16320 // Higgs basis parameters
16321  double dcZHB,cggHB;
16322  double dytHB;
16323  double dKlambda;
16324 
16325  dcZHB = deltacZ_HB();
16326  cggHB = cgg_HB();
16327  dytHB = deltayt_HB();
16328  dKlambda = deltaG_hhhRatio();
16329 
16330  double dcZHB2,dcZHB3,dcZHB4;
16331  double cggHB2,cggHB3,cggHB4;
16332  double dytHB2,dytHB3,dytHB4,dytHB5,dytHB6,dytHB7,dytHB8;
16333  double dKlambda2,dKlambda3,dKlambda4;
16334 
16335  dcZHB2 = dcZHB * dcZHB;
16336  dcZHB3 = dcZHB2 * dcZHB;
16337  dcZHB4 = dcZHB3 * dcZHB;
16338 
16339  cggHB2 = cggHB * cggHB;
16340  cggHB3 = cggHB2 * cggHB;
16341  cggHB4 = cggHB3 * cggHB;
16342 
16343  dytHB2 = dytHB * dytHB;
16344  dytHB3 = dytHB2 * dytHB;
16345  dytHB4 = dytHB3 * dytHB;
16346  dytHB5 = dytHB4 * dytHB;
16347  dytHB6 = dytHB5 * dytHB;
16348  dytHB7 = dytHB6 * dytHB;
16349  dytHB8 = dytHB7 * dytHB;
16350 
16351  dKlambda2 = dKlambda * dKlambda;
16352  dKlambda3 = dKlambda2 * dKlambda;
16353  dKlambda4 = dKlambda3 * dKlambda;
16354 
16355  // The Chi2
16356 
16357  Chi2Tot = 2.0595082782796297e7 * cggHB2 - 3.6971136499764752e9 * cggHB3 + 1.7583900534677216e11 * cggHB4
16358  - 630035.4483047676 * cggHB * dcZHB + 1.3588174266991532e8 * cggHB2 * dcZHB - 7.10364464231958e9 * cggHB3 * dcZHB
16359  + 5311.651853836387 * dcZHB2 - 1.7067170379207395e6 * cggHB * dcZHB2 + 1.1851653627034137e8 * cggHB2 * dcZHB2
16360  + 8180.119549200313 * dcZHB3 - 943018.2335425722 * cggHB * dcZHB3 + 3159.9135213745994 * dcZHB4
16361  + 180518.97210352542 * cggHB * dKlambda - 2.8949546963646576e7 * cggHB2 * dKlambda - 5.501576225306801e8 * cggHB3 * dKlambda
16362  + 1.5079027448500854e11 * cggHB4 * dKlambda - 2846.9365320948145 * dcZHB * dKlambda + 797208.485191074 * cggHB * dcZHB * dKlambda
16363  - 4.978486710457227e6 * cggHB2 * dcZHB * dKlambda - 4.586348042437428e9 * cggHB3 * dcZHB * dKlambda - 6485.875373880575 * dcZHB2 * dKlambda
16364  + 390177.86145601963 * cggHB * dcZHB2 * dKlambda + 5.056678567468029e7 * cggHB2 * dcZHB2 * dKlambda - 3291.6842405815532 * dcZHB3 * dKlambda
16365  - 198301.99217208195 * cggHB * dcZHB3 * dKlambda + 399.29685823653153 * dKlambda2 - 95580.41780509672 * cggHB * dKlambda2
16366  - 7.430874086734321e6 * cggHB2 * dKlambda2 + 7.720064658809748e8 * cggHB3 * dKlambda2 + 5.089872992160051e10 * cggHB4 * dKlambda2
16367  + 1809.9095844013955 * dcZHB * dKlambda2 - 1150.4119995786175 * cggHB * dcZHB * dKlambda2 - 2.2786176268418655e7 * cggHB2 * dcZHB * dKlambda2
16368  - 1.0351049455121036e9 * cggHB3 * dcZHB * dKlambda2 + 1362.5781363223641 * dcZHB2 * dKlambda2 + 170792.06609378837 * cggHB * dcZHB2 * dKlambda2
16369  + 5.658917948194164e6 * cggHB2 * dcZHB2 * dKlambda2 - 178.77181321253659 * dKlambda3 - 11443.938844928987 * cggHB * dKlambda3
16370  + 2.461878722072089e6 * cggHB2 * dKlambda3 + 2.821167791764089e8 * cggHB3 * dKlambda3 + 7.998289700049803e9 * cggHB4 * dKlambda3
16371  - 267.7615464146533 * dcZHB * dKlambda3 - 52488.33374581051 * cggHB * dcZHB * dKlambda3 - 3.555711022595523e6 * cggHB2 * dcZHB * dKlambda3
16372  - 8.149153208622633e7 * cggHB3 * dcZHB * dKlambda3 + 21.07398490236267 * dKlambda4 + 5735.3996792942135 * cggHB * dKlambda4
16373  + 596986.3215027236 * cggHB2 * dKlambda4 + 2.773647081412465e7 * cggHB3 * dKlambda4 + 4.915460918180312e8 * cggHB4 * dKlambda4
16374  + 740876.8879497008 * cggHB * dytHB - 1.938279550686329e8 * cggHB2 * dytHB + 1.1944585224312653e10 * cggHB3 * dytHB
16375  - 12947.635844899749 * dcZHB * dytHB + 4.908519506685015e6 * cggHB * dcZHB * dytHB - 3.742271337006843e8 * cggHB2 * dcZHB * dytHB
16376  - 33546.241370498166 * dcZHB2 * dytHB + 4.3134482870087875e6 * cggHB * dcZHB2 * dytHB - 18267.038917513022 * dcZHB3 * dytHB
16377  + 3387.385955080094 * dKlambda * dytHB - 963072.1570381082 * cggHB * dKlambda * dytHB - 2.3453010760683898e7 * cggHB2 * dKlambda * dytHB
16378  + 9.317798790237669e9 * cggHB3 * dKlambda * dytHB + 14461.190498065112 * dcZHB * dKlambda * dytHB - 276210.0620250288 * cggHB * dcZHB * dKlambda * dytHB
16379  - 2.1850896154428744e8 * cggHB2 * dcZHB * dKlambda * dytHB + 7442.375770947524 * dcZHB2 * dKlambda * dytHB
16380  + 1.6339998473341048e6 * cggHB * dcZHB2 * dKlambda * dytHB - 3291.6842405815532 * dcZHB3 * dKlambda * dytHB - 1559.6600507789517 * dKlambda2 * dytHB
16381  - 212800.20942464058 * cggHB * dKlambda2 * dytHB + 3.499621075016396e7 * cggHB2 * dKlambda2 * dytHB + 2.9495867407085886e9 * cggHB3 * dKlambda2 * dytHB
16382  - 132.54584108464164 * dcZHB * dKlambda2 * dytHB - 704650.5551856682 * cggHB * dcZHB * dKlambda2 * dytHB
16383  - 4.6230021860231325e7 * cggHB2 * dcZHB * dKlambda2 * dytHB + 2725.1562726447282 * dcZHB2 * dKlambda2 * dytHB
16384  + 170792.06609378837 * cggHB * dcZHB2 * dKlambda2 * dytHB - 174.87036642817392 * dKlambda3 * dytHB + 72002.66692264378 * cggHB * dKlambda3 * dytHB
16385  + 1.2160354917437742e7 * cggHB2 * dKlambda3 * dytHB + 4.500393455278235e8 * cggHB3 * dKlambda3 * dytHB - 803.2846392439599 * dcZHB * dKlambda3 * dytHB
16386  - 104976.66749162102 * cggHB * dcZHB * dKlambda3 * dytHB - 3.555711022595523e6 * cggHB2 * dcZHB * dKlambda3 * dytHB
16387  + 84.29593960945068 * dKlambda4 * dytHB + 17206.19903788264 * cggHB * dKlambda4 * dytHB + 1.1939726430054472e6 * cggHB2 * dKlambda4 * dytHB
16388  + 2.773647081412465e7 * cggHB3 * dKlambda4 * dytHB + 7985.615632692477 * dytHB2 - 4.312707242837639e6 * cggHB * dytHB2
16389  + 4.446488644358661e8 * cggHB2 * dytHB2 - 5.669235052669609e9 * cggHB3 * dytHB2 + 59322.05816648064 * dcZHB * dytHB2
16390  - 1.0048203483978426e7 * cggHB * dcZHB * dytHB2 + 2.009903412514487e8 * cggHB2 * dcZHB * dytHB2 + 64971.66315898899 * dcZHB2 * dytHB2
16391  - 2.4669987769536236e6 * cggHB * dcZHB2 * dytHB2 + 11471.803789781865 * dcZHB3 * dytHB2 - 11811.249755773804 * dKlambda * dytHB2
16392  + 431747.7364057698 * cggHB * dKlambda * dytHB2 + 2.2358583287946397e8 * cggHB2 * dKlambda * dytHB2 - 3.8910877145439386e9 * cggHB3 * dKlambda * dytHB2
16393  - 16029.606555240167 * dcZHB * dKlambda * dytHB2 - 2.9253661324121524e6 * cggHB * dcZHB * dKlambda * dytHB2
16394  + 8.987023921425158e7 * cggHB2 * dcZHB * dKlambda * dytHB2 + 4717.219498302798 * dcZHB2 * dKlambda * dytHB2
16395  - 540895.9436706528 * cggHB * dcZHB2 * dKlambda * dytHB2 + 214.81067429237223 * dKlambda2 * dytHB2 + 567954.341114266 * cggHB * dKlambda2 * dytHB2
16396  + 4.5123619667514816e7 * cggHB2 * dKlambda2 * dytHB2 - 9.277345617086976e8 * cggHB3 * dKlambda2 * dytHB2
16397  - 3081.626211728115 * dcZHB * dKlambda2 * dytHB2 - 381097.4778098703 * cggHB * dcZHB * dKlambda2 * dytHB2
16398  + 1.050966209735231e7 * cggHB2 * dcZHB * dKlambda2 * dytHB2 + 1362.5781363223641 * dcZHB2 * dKlambda2 * dytHB2
16399  + 284.9520271687106 * dKlambda3 * dytHB2 + 127206.63260007375 * cggHB * dKlambda3 * dytHB2 + 6.267940600872645e6 * cggHB2 * dKlambda3 * dytHB2
16400  - 7.655202990726441e7 * cggHB3 * dKlambda3 * dytHB2 - 803.2846392439599 * dcZHB * dKlambda3 * dytHB2 - 52488.33374581051 * cggHB * dcZHB * dKlambda3 * dytHB2
16401  + 126.44390941417602 * dKlambda4 * dytHB2 + 17206.19903788264 * cggHB * dKlambda4 * dytHB2 + 596986.3215027236 * cggHB2 * dKlambda4 * dytHB2
16402  - 37223.626257417236 * dytHB3 + 8.269994128894571e6 * cggHB * dytHB3 - 2.9221928856272686e8 * cggHB2 * dytHB3 - 105038.22976459829 * dcZHB * dytHB3
16403  + 7.149383019204844e6 * cggHB * dcZHB * dytHB3 - 47474.492515326274 * dcZHB2 * dytHB3 + 11656.27418420629 * dKlambda * dytHB3
16404  + 2.385352845620739e6 * cggHB * dKlambda * dytHB3 - 1.8438201632292444e8 * cggHB2 * dKlambda * dytHB3 - 8524.8765354653 * dcZHB * dKlambda * dytHB3
16405  + 2.8867300035650665e6 * cggHB * dcZHB * dKlambda * dytHB3 - 9211.031646525304 * dcZHB2 * dKlambda * dytHB3 + 3263.1999469874036 * dKlambda2 * dytHB3
16406  + 44138.45406924717 * cggHB * dKlambda2 * dytHB3 - 4.193837918690795e7 * cggHB2 * dKlambda2 * dytHB3 + 1474.023437403278 * dcZHB * dKlambda2 * dytHB3
16407  + 322402.6653762193 * cggHB * dcZHB * dKlambda2 * dytHB3 + 116.36014794980927 * dKlambda3 * dytHB3 - 7370.4909474997985 * cggHB * dKlambda3 * dytHB3
16408  - 3.4305355944930054e6 * cggHB2 * dKlambda3 * dytHB3 - 267.7615464146533 * dcZHB * dKlambda3 * dytHB3 + 84.29593960945068 * dKlambda4 * dytHB3
16409  + 5735.3996792942135 * cggHB * dKlambda4 * dytHB3 + 66652.27308402126 * dytHB4 - 6.871040436399154e6 * cggHB * dytHB4
16410  + 9.22099747455498e7 * cggHB2 * dytHB4 + 92021.78032189047 * dcZHB * dytHB4 - 2.257899878309953e6 * cggHB * dcZHB * dytHB4
16411  + 16245.693309808961 * dcZHB2 * dytHB4 + 2838.4331580144003 * dKlambda * dytHB4 - 2.731422853592693e6 * cggHB * dKlambda * dytHB4
16412  + 4.274439860749665e7 * cggHB2 * dKlambda * dytHB4 + 15892.926730807862 * dcZHB * dKlambda * dytHB4 - 515009.5486394962 * cggHB * dcZHB * dKlambda * dytHB4
16413  - 1056.6073875703482 * dKlambda2 * dytHB4 - 482475.3464808796 * cggHB * dKlambda2 * dytHB4 + 5.170468004804585e6 * cggHB2 * dKlambda2 * dytHB4
16414  + 2613.194223645355 * dcZHB * dKlambda2 * dytHB4 - 427.75818525652596 * dKlambda3 * dytHB4 - 51130.51778000078 * cggHB * dKlambda3 * dytHB4
16415  + 21.07398490236267 * dKlambda4 * dytHB4 - 63203.969008703876 * dytHB5 + 3.151938475204292e6 * cggHB * dytHB5 - 42834.09620756765 * dcZHB * dytHB5
16416  - 12524.979109927113 * dKlambda * dytHB5 + 1.3421161655790398e6 * cggHB * dKlambda * dytHB5 - 8919.930319126936 * dcZHB * dKlambda * dytHB5
16417  - 849.49051561947 * dKlambda2 * dytHB5 + 158560.3321836832 * cggHB * dKlambda2 * dytHB5 - 263.0677528219873 * dKlambda3 * dytHB5
16418  + 37913.4502786983 * dytHB6 - 712582.2268647491 * cggHB * dytHB6 + 10593.332328402174 * dcZHB * dytHB6 + 8514.598993531516 * dKlambda * dytHB6
16419  - 169200.83566434312 * cggHB * dKlambda * dytHB6 + 1296.5492356304262 * dKlambda2 * dytHB6 - 13281.426292006341 * dytHB7
16420  - 2976.898633587163 * dKlambda * dytHB7 + 2684.433665848417 * dytHB8;
16421 
16422  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16423  return sqrt(Chi2Tot);
16424 }

◆ AuxObs_NP15()

double NPSMEFTd6::AuxObs_NP15 ( ) const
virtual

Auxiliary observable AuxObs_NP15.

Returns
AuxObs_NP15

Reimplemented from NPbase.

Definition at line 16426 of file NPSMEFTd6.cpp.

16427 {
16428  // To be used for some temporary observable
16429  return 0.0;
16430 }

◆ AuxObs_NP16()

double NPSMEFTd6::AuxObs_NP16 ( ) const
virtual

Auxiliary observable AuxObs_NP16.

Returns
AuxObs_NP16

Reimplemented from NPbase.

Definition at line 16432 of file NPSMEFTd6.cpp.

16433 {
16434  // To be used for some temporary observable
16435  return 0.0;
16436 }

◆ AuxObs_NP17()

double NPSMEFTd6::AuxObs_NP17 ( ) const
virtual

Auxiliary observable AuxObs_NP17.

Returns
AuxObs_NP17

Reimplemented from NPbase.

Definition at line 16438 of file NPSMEFTd6.cpp.

16439 {
16440  // To be used for some temporary observable
16441  return 0.0;
16442 }

◆ AuxObs_NP18()

double NPSMEFTd6::AuxObs_NP18 ( ) const
virtual

Auxiliary observable AuxObs_NP18.

Returns
AuxObs_NP18

Reimplemented from NPbase.

Definition at line 16444 of file NPSMEFTd6.cpp.

16445 {
16446  // To be used for some temporary observable
16447  return 0.0;
16448 }

◆ AuxObs_NP19()

double NPSMEFTd6::AuxObs_NP19 ( ) const
virtual

Auxiliary observable AuxObs_NP19.

Returns
AuxObs_NP19

Reimplemented from NPbase.

Definition at line 16450 of file NPSMEFTd6.cpp.

16451 {
16452  // To be used for some temporary observable
16453  return 0.0;
16454 }

◆ AuxObs_NP2()

double NPSMEFTd6::AuxObs_NP2 ( ) const
virtual

Auxiliary observable AuxObs_NP2 (See code for details.)

Returns
AuxObs_NP2

Reimplemented from NPbase.

Definition at line 15646 of file NPSMEFTd6.cpp.

15647 {
15648  // To be used for some temporary observable
15649 
15650  // WY analysis at 13 TeV for HL-LHC 3/ab for the CC
15651  // WY analysis at 27 TeV for HE-LHC 15/ab for the NC. 5% systematics (corr and uncorr)
15652  double Wpar, Ypar, Wpar2, Ypar2;
15653  double Chi2NC27, Chi2CC13, Chi2Tot;
15654 
15655  Wpar = 10000.0 * obliqueW();
15656  Ypar = 10000.0 * obliqueY();
15657 
15658  Wpar2 = Wpar*Wpar;
15659  Ypar2 = Ypar*Ypar;
15660 
15661  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
15662 
15663  Chi2NC27 = 21.139285368181907 * Wpar2*Wpar2 + Wpar2*Wpar * (-89.16828370317616 + 7.182929295852857 * Ypar)
15664  + Wpar * Ypar * (208.8092257396059 + Ypar * (-81.00102926445666 + 6.203591096144735 * Ypar))
15665  + Ypar2 * (81.01075991905888 + Ypar * (-58.822719932531164 + 14.670206406369107 * Ypar))
15666  + Wpar2 * (136.70787790194357 + Ypar * (-86.48485007990255 + 35.67671393730628 * Ypar));
15667 
15668  Chi2Tot = Chi2CC13 + Chi2NC27;
15669 
15670  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15671  return sqrt(Chi2Tot);
15672 }

◆ AuxObs_NP20()

double NPSMEFTd6::AuxObs_NP20 ( ) const
virtual

Auxiliary observable AuxObs_NP20.

Returns
AuxObs_NP20

Reimplemented from NPbase.

Definition at line 16456 of file NPSMEFTd6.cpp.

16457 {
16458  // To be used for some temporary observable
16459  return 0.0;
16460 }

◆ AuxObs_NP3()

double NPSMEFTd6::AuxObs_NP3 ( ) const
virtual

Auxiliary observable AuxObs_NP3 (See code for details.)

Returns
AuxObs_NP3

Reimplemented from NPbase.

Definition at line 15674 of file NPSMEFTd6.cpp.

15675 {
15676  // To be used for some temporary observable
15677 
15678  // WY analysis at 13 TeV for HL-LHC 3/ab for the CC
15679  // WY analysis at 27 TeV for HE-LHC 15/ab for the NC. 1% systematics (corr and uncorr)
15680  double Wpar, Ypar, Wpar2, Ypar2;
15681  double Chi2NC27, Chi2CC13, Chi2Tot;
15682 
15683  Wpar = 10000.0 * obliqueW();
15684  Ypar = 10000.0 * obliqueY();
15685 
15686  Wpar2 = Wpar*Wpar;
15687  Ypar2 = Ypar*Ypar;
15688 
15689  Chi2CC13 = Wpar2 * (18.365037149441695 + 2.422904241798858 * Wpar + 0.12120594308623695 * Wpar2);
15690 
15691  Chi2NC27 = 25.148424251427552 * Wpar2*Wpar2 + Wpar2*Wpar * (-105.31753344410277 + 8.01723084630248 * Ypar)
15692  + Wpar * Ypar * (253.11721255992683 + Ypar * (-93.18990615818014 + 6.8250043104055816 * Ypar))
15693  + Ypar2 * (97.52107126224298 + Ypar * (-67.961770347904945 + 16.80046890875678 * Ypar))
15694  + Wpar2 * (166.84179829911304 + Ypar * (-100.88118582829852 + 41.55424691040131 * Ypar));
15695 
15696  Chi2Tot = Chi2CC13 + Chi2NC27;
15697 
15698  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15699  return sqrt(Chi2Tot);
15700 }

◆ AuxObs_NP4()

double NPSMEFTd6::AuxObs_NP4 ( ) const
virtual

Auxiliary observable AuxObs_NP4 (See code for details.)

Returns
AuxObs_NP4

Reimplemented from NPbase.

Definition at line 15702 of file NPSMEFTd6.cpp.

15703 {
15704  // WH distribution at 14 TeV: From 1704.01953 + hvqq terms
15705 
15706  double Bin1 = 1.0, Bin2 = 1.0, Bin3 = 1.0, Bin4 = 1.0, Bin5 = 1.0;
15707 
15708  double dVud = 0.0, dVcs = 0.0;
15709  double dcZ = 0.0, cZBox = 0.0, cZZ = 0.0, cZA = 0.0, cAA = 0.0;
15710 
15711  double C11 = 0.0178, C12 = 0.0144, C13 = 0.0102, C14 = 0.0052, C15 = 0.0006;
15712 
15713  double dchi2;
15714 
15715 // Production in each bin (signal strength)
15716 
15717  Bin1 += 12.8 * dVud + 1.75 * dVcs
15718  + 2.00 * dcZ + 5.01 * cZBox + 2.72 * cZZ - 0.0267 * cZA - 0.0217 * cAA;
15719 
15720 // Linear contribution from Higgs self-coupling
15721  Bin1 = Bin1 + cLHd6*(C11 + 2.0*dZH)*deltaG_hhhRatio();
15722 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15723  Bin1 = Bin1 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15724 
15725  Bin2 += 15.3 * dVud + 1.91 * dVcs
15726  + 2.00 * dcZ + 5.81 * cZBox + 3.10 * cZZ - 0.0337 * cZA - 0.0255 * cAA;
15727 
15728 // Linear contribution from Higgs self-coupling
15729  Bin2 = Bin2 + cLHd6*(C12 + 2.0*dZH)*deltaG_hhhRatio();
15730 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15731  Bin2 = Bin2 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15732 
15733  Bin3 += 20.7 * dVud + 2.49 * dVcs
15734  + 2.01 * dcZ + 7.44 * cZBox + 3.76 * cZZ - 0.0535 * cZA - 0.0340 * cAA;
15735 
15736 // Linear contribution from Higgs self-coupling
15737  Bin3 = Bin3 + cLHd6*(C13 + 2.0*dZH)*deltaG_hhhRatio();
15738 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15739  Bin3 = Bin3 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15740 
15741  Bin4 += 35.1 * dVud + 3.63 * dVcs
15742  + 1.98 * dcZ + 11.8 * cZBox + 5.40 * cZZ - 0.112 * cZA - 0.0572 * cAA;
15743 
15744 // Linear contribution from Higgs self-coupling
15745  Bin4 = Bin4 + cLHd6*(C14 + 2.0*dZH)*deltaG_hhhRatio();
15746 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15747  Bin4 = Bin4 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15748 
15749  Bin5 += 67.7 * dVud + 5.41 * dVcs
15750  + 2.03 * dcZ + 22.6 * cZBox + 9.05 * cZZ - 0.276 * cZA - 0.117 * cAA;
15751 
15752 // Linear contribution from Higgs self-coupling
15753  Bin5 = Bin5 + cLHd6*(C15 + 2.0*dZH)*deltaG_hhhRatio();
15754 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15755  Bin5 = Bin5 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15756 
15757 // Compute Chi square using only the last bin and the diphoton, ZZ and bb channels
15758  dchi2 = ( Bin5 * BrHZZ4lRatio() - 1.0 ) * ( Bin5 * BrHZZ4lRatio() - 1.0 )/(0.07*0.07 + 0.48*0.48)
15759  + ( Bin5 * BrHgagaRatio() - 1.0 ) * ( Bin5 * BrHgagaRatio() - 1.0 )/(0.08*0.08 + 0.54*0.54)
15760  + ( Bin5 * BrHbbRatio() - 1.0 ) * ( Bin5 * BrHbbRatio() - 1.0 )/(0.33*0.33 + 0.61*0.61);
15761 
15762  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15763  return sqrt(dchi2);
15764 }

◆ AuxObs_NP5()

double NPSMEFTd6::AuxObs_NP5 ( ) const
virtual

Auxiliary observable AuxObs_NP5 (See code for details.)

Returns
AuxObs_NP5

Reimplemented from NPbase.

Definition at line 15766 of file NPSMEFTd6.cpp.

15767 {
15768  // ZH distribution at 14 TeV: From 1704.01953 + hvqq terms
15769 
15770  double Bin1 = 1.0, Bin2 = 1.0, Bin3 = 1.0, Bin4 = 1.0, Bin5 = 1.0;
15771 
15772  double dgLZuu = 0.0, dgRZuu = 0.0, dgLZcc = 0.0, dgRZcc = 0.0;
15773  double dgLZdd = 0.0, dgRZdd = 0.0, dgLZss = 0.0, dgRZss = 0.0;
15774 
15775  double dcZ = 0.0, cZBox = 0.0, cZZ = 0.0, cZA = 0.0, cAA = 0.0;
15776 
15777  double C11 = 0.0208, C12 = 0.0164, C13 = 0.0112, C14 = 0.0051, C15 = 0.0021;
15778 
15779  double dchi2;
15780 
15781 // Production in each bin (signal strength)
15782 
15783  Bin1 += 14.6 * dgLZuu - 6.74 * dgRZuu - 11.6 * dgLZdd + 2.28 * dgRZdd
15784  + 1.35 * dgLZcc - 0.589 * dgRZcc - 2.35 * dgLZss + 0.431 * dgRZss
15785  + 2.01 * dcZ + 4.14 * cZBox + 2.12 * cZZ - 0.0237 * cZA - 0.0126 * cAA;
15786 
15787 // Linear contribution from Higgs self-coupling
15788  Bin1 = Bin1 + cLHd6*(C11 + 2.0*dZH)*deltaG_hhhRatio();
15789 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15790  Bin1 = Bin1 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15791 
15792  Bin2 += 16.2 * dgLZuu - 7.77 * dgRZuu - 13.4 * dgLZdd + 2.63 * dgRZdd
15793  + 1.44 * dgLZcc - 0.668 * dgRZcc - 2.52 * dgLZss + 0.462 * dgRZss
15794  + 2.01 * dcZ + 4.86* cZBox + 2.49 * cZZ - 0.0284 * cZA - 0.0156 * cAA;
15795 
15796 // Linear contribution from Higgs self-coupling
15797  Bin2 = Bin2 + cLHd6*(C12 + 2.0*dZH)*deltaG_hhhRatio();
15798 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15799  Bin2 = Bin2 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15800 
15801  Bin3 += 23.0* dgLZuu - 10.8 * dgRZuu - 19.0 * dgLZdd + 3.64 * dgRZdd
15802  + 1.88 * dgLZcc - 0.891 * dgRZcc - 3.19 * dgLZss + 0.591 * dgRZss
15803  + 2.00 * dcZ + 6.35 * cZBox + 3.02 * cZZ - 0.0448 * cZA - 0.0221 * cAA;
15804 
15805 // Linear contribution from Higgs self-coupling
15806  Bin3 = Bin3 + cLHd6*(C13 + 2.0*dZH)*deltaG_hhhRatio();
15807 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15808  Bin3 = Bin3 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15809 
15810  Bin4 += 39.2 * dgLZuu - 18.4 * dgRZuu - 31.4 * dgLZdd + 5.88 * dgRZdd
15811  + 2.78 * dgLZcc - 1.36 * dgRZcc - 4.64 * dgLZss + 0.919 * dgRZss
15812  + 1.98 * dcZ + 10.5 * cZBox + 4.44 * cZZ - 0.0873 * cZA - 0.0396 * cAA;
15813 
15814 // Linear contribution from Higgs self-coupling
15815  Bin4 = Bin4 + cLHd6*(C14 + 2.0*dZH)*deltaG_hhhRatio();
15816 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15817  Bin4 = Bin4 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15818 
15819  Bin5 += 73.4 * dgLZuu - 35.5 * dgRZuu - 58.5 * dgLZdd + 11.2 * dgRZdd
15820  + 4.13 * dgLZcc - 1.95 * dgRZcc - 6.97 * dgLZss + 1.41 * dgRZss
15821  + 1.96 * dcZ + 20.3 * cZBox + 7.27 * cZZ - 0.193 * cZA - 0.0800 * cAA;
15822 
15823 // Linear contribution from Higgs self-coupling
15824  Bin5 = Bin5 + cLHd6*(C15 + 2.0*dZH)*deltaG_hhhRatio();
15825 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
15826  Bin5 = Bin5 + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
15827 
15828 // Compute Chi square using only the last bin and the diphoton, ZZ and bb channels
15829  dchi2 = ( Bin5 * BrHZZ4lRatio() - 1.0 ) * ( Bin5 * BrHZZ4lRatio() - 1.0 )/(0.09*0.09 + 0.65*0.65)
15830  + ( Bin5 * BrHgagaRatio() - 1.0 ) * ( Bin5 * BrHgagaRatio() - 1.0 )/(0.03*0.03 + 0.99*0.99)
15831  + ( Bin5 * BrHbbRatio() - 1.0 ) * ( Bin5 * BrHbbRatio() - 1.0 )/(0.10*0.10 + 0.34*0.34);
15832 
15833  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
15834  return sqrt(dchi2);
15835 }

◆ AuxObs_NP6()

double NPSMEFTd6::AuxObs_NP6 ( ) const
virtual

Auxiliary observable AuxObs_NP6 (See code for details.)

Returns
AuxObs_NP6

Reimplemented from NPbase.

Definition at line 15837 of file NPSMEFTd6.cpp.

15838 {
15839  // To be used for some temporary observable
15840 
15841  // HL-LHC DiHiggs invariant mass distribution: 14 TeV 3/ab
15842 
15843  double Chi2Tot;
15844 
15845 // NP in decays
15846  double dGH2,dGgaga,dGbb, dBRTot;
15847 
15848 // Contributions from the different bins
15849  double Bin1,Bin2,Bin3,Bin4,Bin5,Bin6;
15850  double LLBin1, LLBin2, LLBin3, LLBin4, LLBin5, LLBin6;
15851 
15852 // Higgs basis parameters
15853  double dcZHB,cZboxHB,cZZHB,cZgaHB,cgagaHB,cggHB;
15854  double dytHB,dybHB,dytauHB;
15855  double dKlambda;
15856 
15857  dcZHB = deltacZ_HB();
15858  cZboxHB = cZBox_HB();
15859  cZZHB = cZZ_HB();
15860 
15861 // In the paper it seems they use diff. norm but in the chi 2.nb
15862 // they translate into that convention, so I assume their calculation
15863 // is directly in the HB for the following 3 couplings
15864  cZgaHB = cZga_HB();
15865  cgagaHB = cgaga_HB();
15866  cggHB = cgg_HB();
15867 
15868  dytHB = deltayt_HB();
15869  dybHB = deltayb_HB();
15870  dytauHB = deltaytau_HB();
15871 
15872  dKlambda = deltaG_hhhRatio();
15873 
15874 // Corrections to the different Higgs widths
15875  dGH2 = 1. + 0.010512791990056657 * cZboxHB
15876  - 0.003819752423722165 * cZZHB + 0.0016024991450954641 * cZgaHB
15877  - 0.0005968238492400916 * (2.8975474398595105 * cZboxHB
15878  + 1.8975474398595107 * cZZHB - cZgaHB - 0.3426378481886507 * cgagaHB)
15879  + 0.0990750425382019 * (1.4487737199297552 * cZboxHB + 0.44877371992975534 * cZZHB
15880  - 0.2365019764475461 * cZgaHB - 0.08103452830235015 * cgagaHB)
15881  - 0.0330404571742506 * (cZZHB + 0.4730039528950922 * cZgaHB + 0.055933184863595636 * cgagaHB)
15882  - 0.00033171593951211893 * cgagaHB + 0.48287726036165796 * dcZHB
15883  + 1.1541846695471276 * dybHB + 0.12642022723635785 * dytauHB
15884  + 0.1704272683629381 * (0. + 118.68284969347252 * cggHB
15885  - 0.031082871395970327 * dybHB + 1.034601498835783 * dytHB)
15886  + 0.004560729716754681 * (0. - 12.079950077697095 * cgagaHB
15887  + 1.2739859351743013 * dcZHB + 0.0022136399615102554 * dybHB
15888  - 0.28081416399029446 * dytHB + 0.0036305606562964158 * dytauHB)
15889  + 0.003080492878860618 * (0. - 17.021015025105033 * cZgaHB
15890  + 1.0557935963831278 * dcZHB + 0.0006235357344154619 * dybHB
15891  - 0.05644023795399054 * dytHB + 0.000023105836447458856 * dytauHB);
15892 
15893  dGH2 = dGH2 * dGH2;
15894 
15895  dGgaga = 1.0 + 2.0 * (0. - 12.079950077697095 * cgagaHB
15896  + 1.2739859351743013 * dcZHB + 0.0022136399615102554 * dybHB
15897  - 0.28081416399029446 * dytHB + 0.0036305606562964158 * dytauHB);
15898 
15899  dGbb = 1.0 + 2.0 * dybHB;
15900 
15901  dBRTot = dGbb * dGgaga / dGH2;
15902 
15903  // Bin 1
15904  Bin1 = 0.17*(1.0 + 3.9863794294589585 * cggHB
15905  + 21.333394807321064 * cggHB*cggHB + 3.9527789724382836 * dcZHB
15906  + 0.5566823785534646 * cggHB*dcZHB + 9.077153576669469 * dcZHB*dcZHB
15907  - 7.713285621354339 * dytHB + 6.573887966178747 * cggHB*dytHB
15908  - 45.88983201032187 * dcZHB*dytHB + 62.42156375416841 * dytHB*dytHB
15909  + 4.257555672380181 * cggHB*dytHB*dytHB + 4.620310477256665 * dcZHB*dytHB*dytHB
15910  - 9.403185493195476 * dytHB*dytHB*dytHB + 1.1563473213070041 * dytHB*dytHB*dytHB*dytHB
15911  - 0.14505129596051047 * dKlambda - 0.1418831193390564 * cggHB*dKlambda
15912  + 1.3502693869386464 * cggHB*cggHB*dKlambda - 0.6675315048183816 * dcZHB*dKlambda
15913  - 0.002999558395846163 * cggHB*dcZHB*dKlambda
15914  + 1.5448485758806263 * dytHB * dKlambda
15915  - 0.005002986050963205 * cggHB*dytHB*dKlambda
15916  - 0.6675315048183816 * dcZHB*dytHB * dKlambda
15917  + 1.5222565251876392 * dytHB*dytHB * dKlambda
15918  + 0.1278814581005547 * cggHB*dytHB*dytHB * dKlambda
15919  - 0.1676433466534976 * dytHB*dytHB*dytHB * dKlambda
15920  + 0.011296025346493552 * dKlambda*dKlambda
15921  + 0.0014116654816114353 * cggHB*dKlambda*dKlambda
15922  + 0.022260157195710357 * cggHB*cggHB*dKlambda*dKlambda
15923  + 0.022592050692987104 * dytHB * dKlambda*dKlambda
15924  + 0.0014116654816114353 * cggHB*dytHB*dKlambda*dKlambda
15925  + 0.011296025346493552 * dytHB*dytHB * dKlambda*dKlambda);
15926 
15927  Bin1 = 0.67944 + Bin1 * dBRTot;
15928 
15929  // Exclude points with negative values of BinX
15930  if ( Bin1 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15931 
15932  // Delta chi2 = -2*LL for the bin
15933  // Add an abs in the denominator of the log,
15934  // even if events with negative BinX are not supposed to reach here.
15935  LLBin1 = 2.0 * (Bin1 - 0.84944 + 0.84944 * log( 0.84944 / fabs(Bin1) ) );
15936 
15937  // Bin 2
15938  Bin2 = 0.33*(1.0 + 1.8019627645351037 * cggHB
15939  + 7.953163597932105 * cggHB*cggHB + 3.735123481549394 * dcZHB
15940  - 2.654186900737259 * cggHB*dcZHB + 6.403420811368324 * dcZHB*dcZHB
15941  - 6.991501690350679 * dytHB + 11.425848100026737 * cggHB*dytHB
15942  - 30.219763494155394 * dcZHB*dytHB + 39.692409895713936 * dytHB*dytHB
15943  + 1.661324633279857 * cggHB*dytHB*dytHB + 4.46563789250516 * dcZHB*dytHB*dytHB
15944  - 8.710706509282613 * dytHB*dytHB*dytHB + 1.2361692069676826 * dytHB*dytHB*dytHB*dytHB
15945  - 0.21386875429750188 * dKlambda + 0.2363972133088796 * cggHB*dKlambda
15946  + 0.8549707073528667 * cggHB*cggHB*dKlambda - 0.7305144109557659 * dcZHB*dKlambda
15947  - 0.14136602060890807 * cggHB*dcZHB*dKlambda + 1.50533606463443 * dytHB * dKlambda
15948  + 0.747017712869579 * cggHB*dytHB*dKlambda - 0.7305144109557659 * dcZHB*dytHB * dKlambda
15949  + 1.4607351592940678 * dytHB*dytHB * dKlambda
15950  + 0.08652243773397514 * cggHB*dytHB*dytHB * dKlambda
15951  - 0.25846965963786395 * dytHB*dytHB*dytHB * dKlambda
15952  + 0.022300452670181038 * dKlambda*dKlambda + 0.009236644319657653 * cggHB*dKlambda*dKlambda
15953  + 0.023125582948149842 * cggHB*cggHB*dKlambda*dKlambda
15954  + 0.044600905340362075 * dytHB * dKlambda*dKlambda
15955  + 0.009236644319657653 * cggHB*dytHB*dKlambda*dKlambda
15956  + 0.022300452670181038 * dytHB*dytHB * dKlambda*dKlambda) ;
15957 
15958  Bin2 = 1.4312 + Bin2 * dBRTot;
15959 
15960  // Exclude points with negative values of BinX
15961  if ( Bin2 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15962 
15963  // Delta chi2 = -2*LL for the bin
15964  // Add an abs in the denominator of the log,
15965  // even if events with negative BinX are not supposed to reach here.
15966  LLBin2 = 2.0 * (Bin2 - 1.7612 + 1.7612 * log( 1.7612 / fabs(Bin2) ) );
15967 
15968  // Bin 3
15969  Bin3 = 0.99*(1.0 + 0.6707152151845268 * cggHB
15970  + 4.113022405261353 * cggHB*cggHB + 3.4241906309399726 * dcZHB
15971  - 2.9926046286644703 * cggHB*dcZHB + 4.72026565086762 * dcZHB*dcZHB
15972  - 5.98522416048399 * dytHB + 10.012680455917307 * cggHB*dytHB
15973  - 20.69102310585157 * dcZHB*dytHB + 26.4871108999121 * dytHB*dytHB
15974  + 0.36415135473936855 * cggHB*dytHB*dytHB
15975  + 4.206380168414172 * dcZHB*dytHB*dytHB - 7.688318821918381 * dytHB*dytHB*dytHB
15976  + 1.3217369754941033 * dytHB*dytHB*dytHB*dytHB - 0.2873477323359291 * dKlambda
15977  + 0.35631144357921507 * cggHB*dKlambda
15978  + 0.6197019283831009 * cggHB*cggHB*dKlambda
15979  - 0.7821895374741993 * dcZHB*dKlambda
15980  - 0.23172596419155064 * cggHB*dcZHB*dKlambda
15981  + 1.415746929098462 * dytHB * dKlambda
15982  + 1.0816714186441074 * cggHB*dytHB*dKlambda
15983  - 0.7821895374741993 * dcZHB*dytHB * dKlambda
15984  + 1.3469684427821131 * dytHB*dytHB * dKlambda
15985  + 0.030182082490240562 * cggHB*dytHB*dytHB * dKlambda
15986  - 0.35612621865227795 * dytHB*dytHB*dytHB * dKlambda
15987  + 0.03438924315817444 * dKlambda*dKlambda
15988  + 0.019565500643816278 * cggHB*dKlambda*dKlambda
15989  + 0.02382411268034237 * cggHB*cggHB*dKlambda*dKlambda
15990  + 0.06877848631634888 * dytHB * dKlambda*dKlambda
15991  + 0.019565500643816278 * cggHB*dytHB*dKlambda*dKlambda
15992  + 0.03438924315817444 * dytHB*dytHB * dKlambda*dKlambda);
15993 
15994  Bin3 = 1.9764 + Bin3 * dBRTot;
15995 
15996  // Exclude points with negative values of BinX
15997  if ( Bin3 < 0 ) return std::numeric_limits<double>::quiet_NaN();
15998 
15999  // Delta chi2 = -2*LL for the bin
16000  // Add an abs in the denominator of the log,
16001  // even if events with negative BinX are not supposed to reach here.
16002  LLBin3 = 2.0 * (Bin3 - 2.9664 + 2.9664 * log( 2.9664 / fabs(Bin3) ) );
16003 
16004  // Bin 4
16005  Bin4 = 2.86*(1.0 - 0.27406342847042814 * cggHB
16006  + 1.9597360046161074 * cggHB*cggHB + 3.0113078755334115 * dcZHB
16007  - 2.776019265892887 * cggHB*dcZHB + 3.1917709639679823 * dcZHB*dcZHB
16008  - 4.6362529563760955 * dytHB + 7.377234185667426 * cggHB*dytHB
16009  - 12.294598143269557 * dcZHB*dytHB + 15.407456380301479 * dytHB*dytHB
16010  - 0.6767601835408067 * cggHB*dytHB*dytHB
16011  + 3.844719765004924 * dcZHB*dytHB*dytHB
16012  - 6.227970053277897 * dytHB*dytHB*dytHB + 1.4542592857563688 * dytHB*dytHB*dytHB*dytHB
16013  - 0.39767067022413716 * dKlambda + 0.3661464075997459 * cggHB*dKlambda
16014  + 0.4464409042746693 * cggHB*cggHB*dKlambda
16015  - 0.8334118894715125 * dcZHB*dKlambda
16016  - 0.3263197431214281 * cggHB*dcZHB*dKlambda
16017  + 1.1940464266776625 * dytHB * dKlambda
16018  + 1.2643073873631234 * cggHB*dytHB*dKlambda
16019  - 0.8334118894715125 * dcZHB*dytHB * dKlambda
16020  + 1.0808691956131988 * dytHB*dytHB * dKlambda
16021  - 0.0807982496009068 * cggHB*dytHB*dytHB * dKlambda
16022  - 0.5108479012886007 * dytHB*dytHB*dytHB * dKlambda
16023  + 0.05658861553223176 * dKlambda*dKlambda
16024  + 0.04424790213027415 * cggHB*dKlambda*dKlambda
16025  + 0.02585578262020257 * cggHB*cggHB*dKlambda*dKlambda
16026  + 0.11317723106446352 * dytHB * dKlambda*dKlambda
16027  + 0.04424790213027415 * cggHB*dytHB*dKlambda*dKlambda
16028  + 0.05658861553223176 * dytHB*dytHB * dKlambda*dKlambda);
16029 
16030  Bin4 = 5.167 + Bin4 * dBRTot;
16031 
16032  // Exclude points with negative values of BinX
16033  if ( Bin4 < 0 ) return std::numeric_limits<double>::quiet_NaN();
16034 
16035  // Delta chi2 = -2*LL for the bin
16036  // Add an abs in the denominator of the log,
16037  // even if events with negative BinX are not supposed to reach here.
16038  LLBin4 = 2.0 * (Bin4 - 8.027 + 8.027 * log( 8.027 / fabs(Bin4) ) );
16039 
16040  // Bin 5
16041  Bin5 = 6.34* (1.0 - 1.094329254675176 * cggHB
16042  + 1.0393648302909912 * cggHB*cggHB + 2.6000916816530903 * dcZHB
16043  - 2.4448264513323226 * cggHB*dcZHB + 2.073935963891534 * dcZHB*dcZHB
16044  - 3.192332240205929 * dytHB + 4.5914586198385 * cggHB*dytHB
16045  - 6.2871857258718595 * dcZHB*dytHB + 8.134770266934664 * dytHB*dytHB
16046  - 1.648691479483292 * cggHB*dytHB*dytHB + 3.5563383758242524 * dcZHB*dytHB*dytHB
16047  - 4.615570013047001 * dytHB*dytHB*dytHB + 1.7227511548362076 * dytHB*dytHB*dytHB*dytHB
16048  - 0.6079428047533413 * dKlambda + 0.33825211279194234 * cggHB*dKlambda
16049  + 0.3879052211526028 * cggHB*cggHB*dKlambda - 0.956246694171162 * dcZHB*dKlambda
16050  - 0.4572431444456198 * cggHB*dcZHB*dKlambda + 0.8152949680877302 * dytHB * dKlambda
16051  + 1.3814632626914451 * cggHB*dytHB*dKlambda
16052  - 0.956246694171162 * dcZHB*dytHB * dKlambda + 0.5856782679219981 * dytHB*dytHB * dKlambda
16053  - 0.3285182834373566 * cggHB*dytHB*dytHB * dKlambda
16054  - 0.8375595049190734 * dytHB*dytHB*dytHB * dKlambda + 0.11480835008286604 * dKlambda*dKlambda
16055  + 0.11240817142118299 * cggHB*dKlambda*dKlambda + 0.03688252014841459 * cggHB*cggHB*dKlambda*dKlambda
16056  + 0.22961670016573207 * dytHB * dKlambda*dKlambda
16057  + 0.11240817142118299 * cggHB*dytHB*dKlambda*dKlambda
16058  + 0.11480835008286604 * dytHB*dytHB * dKlambda*dKlambda);
16059 
16060  Bin5 = 15.93 + Bin5 * dBRTot;
16061 
16062  // Exclude points with negative values of BinX
16063  if ( Bin5 < 0 ) return std::numeric_limits<double>::quiet_NaN();
16064 
16065  // Delta chi2 = -2*LL for the bin
16066  // Add an abs in the denominator of the log,
16067  // even if events with negative BinX are not supposed to reach here.
16068  LLBin5 = 2.0 * (Bin5 - 22.27 + 22.27 * log( 22.27 / fabs(Bin5) ) );
16069 
16070  // Bin 6
16071  Bin6 = 2.14*(1.0 - 2.007855065799201 * cggHB + 1.1994575008850934 * cggHB*cggHB
16072  + 2.5987763498382352 * dcZHB - 2.908713303420072 * cggHB*dcZHB
16073  + 1.804645897901265 * dcZHB*dcZHB - 2.806900956988577 * dytHB
16074  + 3.5621616844486415 * cggHB*dytHB - 4.250685020965587 * dcZHB*dytHB
16075  + 5.7468374752045515 * dytHB*dytHB - 3.1561231600123736 * cggHB*dytHB*dytHB
16076  + 3.9784140166037667 * dcZHB*dytHB*dytHB - 4.4303353405513395 * dytHB*dytHB*dytHB
16077  + 2.257739308366916 * dytHB*dytHB*dytHB*dytHB - 0.9894280925261291 * dKlambda
16078  + 0.589956279744333 * cggHB*dKlambda + 0.6687315933211253 * cggHB*cggHB*dKlambda
16079  - 1.3796376667655315 * dcZHB*dKlambda - 0.8069993678124955 * cggHB*dcZHB*dKlambda
16080  + 0.6340062910366335 * dytHB * dKlambda + 2.127573647123277 * cggHB*dytHB*dKlambda
16081  - 1.3796376667655315 * dcZHB*dytHB * dKlambda + 0.09738385935505989 * dytHB*dytHB * dKlambda
16082  - 0.8833807360585424 * cggHB*dytHB*dytHB * dKlambda - 1.5260505242077027 * dytHB*dytHB*dytHB * dKlambda
16083  + 0.2683112158407868 * dKlambda*dKlambda + 0.32506892158970235 * cggHB*dKlambda*dKlambda
16084  + 0.09418943796384227 * cggHB*cggHB*dKlambda*dKlambda + 0.5366224316815736 * dytHB * dKlambda*dKlambda
16085  + 0.32506892158970235 * cggHB*dytHB*dKlambda*dKlambda
16086  + 0.2683112158407868 * dytHB*dytHB * dKlambda*dKlambda);
16087 
16088  Bin6 = 12.01 + Bin6 * dBRTot;
16089 
16090  // Exclude points with negative values of BinX
16091  if ( Bin6 < 0 ) return std::numeric_limits<double>::quiet_NaN();
16092 
16093  // Delta chi2 = -2*LL for the bin
16094  // Add an abs in the denominator of the log,
16095  // even if events with negative BinX are not supposed to reach here.
16096  LLBin6 = 2.0 * (Bin6 - 14.15 + 14.15 * log( 14.15 / fabs(Bin6) ) );
16097 
16098  // The total contributions to the log-likelihood/chi-square
16099  Chi2Tot = LLBin1 + LLBin2 + LLBin3 + LLBin4 + LLBin5 + LLBin6;
16100 
16101  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16102  return sqrt(Chi2Tot);
16103 }

◆ AuxObs_NP7()

double NPSMEFTd6::AuxObs_NP7 ( ) const
virtual

Auxiliary observable AuxObs_NP7 (See code for details.)

Returns
AuxObs_NP7

Reimplemented from NPbase.

Definition at line 16105 of file NPSMEFTd6.cpp.

16106 {
16107  // To be used for some temporary observable
16108 
16109  // CLIC STWY using difermion production at all energies: 380, 1500 and 3000 GeV
16110  double Spar, Tpar, Wpar, Ypar, Spar2, Tpar2, Wpar2, Ypar2;
16111  double Chi2Tot;
16112 
16113  Spar = obliqueS();
16114  Tpar = obliqueT();
16115  Wpar = 10000.0 * obliqueW();
16116  Ypar = 10000.0 * obliqueY();
16117 
16118  Spar2 = Spar*Spar;
16119  Tpar2 = Tpar*Tpar;
16120  Wpar2 = Wpar*Wpar;
16121  Ypar2 = Ypar*Ypar;
16122 
16123  Chi2Tot = 442.84977653097394 * Spar2
16124  - 728.5215604181935 * Spar * Tpar
16125  + 404.15957807101813 * Tpar2
16126  + 400.03987723904224 * Spar * Wpar
16127  - 639.6154242400826 * Tpar * Wpar
16128  + 4337.791457515823 * Wpar2
16129  - 106.87313892453362 * Spar * Ypar
16130  - 72.94355609762007 * Tpar * Ypar
16131  + 3002.848116515672 * Wpar * Ypar
16132  + 3040.1630882458923 * Ypar2;
16133 
16134  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16135  return sqrt(Chi2Tot);
16136 }

◆ AuxObs_NP8()

double NPSMEFTd6::AuxObs_NP8 ( ) const
virtual

Auxiliary observable AuxObs_NP8 (See code for details.)

Returns
AuxObs_NP8

Reimplemented from NPbase.

Definition at line 16138 of file NPSMEFTd6.cpp.

16139 {
16140  // To be used for some temporary observable
16141 
16142  // CLIC DiHiggs: exclusive analysis. Full CLIC run
16143  double Chi2Tot;
16144 
16145 // Higgs basis parameters
16146  double dKlambda;
16147 
16148  dKlambda = deltaG_hhhRatio();
16149 
16150  Chi2Tot = dKlambda * dKlambda * (50.04473972806045
16151  - 104.47283225861888 * dKlambda
16152  + 84.48333683635175 * dKlambda*dKlambda );
16153 
16154  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16155  return sqrt(Chi2Tot);
16156 }

◆ AuxObs_NP9()

double NPSMEFTd6::AuxObs_NP9 ( ) const
virtual

Auxiliary observable AuxObs_NP9 (See code for details.)

Returns
AuxObs_NP9

Reimplemented from NPbase.

Definition at line 16158 of file NPSMEFTd6.cpp.

16159 {
16160  // To be used for some temporary observable
16161 
16162  // ILC DiHiggs at 500 GeV: 2/ab per polarization (+-80,-+30)
16163 
16164  double Chi2p80m30, Chi2m80p30, Chi2Tot;
16165 
16166 // Higgs basis parameters
16167  double dcZHB,cZboxHB,cZZHB,cZgaHB,cgagaHB;
16168  double dKlambda;
16169 
16170  dcZHB = deltacZ_HB();
16171  cZboxHB = cZBox_HB();
16172  cZZHB = cZZ_HB();
16173  cZgaHB = cZga_HB();
16174  cgagaHB = cgaga_HB();
16175 
16176  dKlambda = deltaG_hhhRatio();
16177 
16178 // The signal strength -1
16179  Chi2p80m30 = 13.6982 * cZZHB
16180  - 7.58943 * cZgaHB
16181  + 14.6843 * cZboxHB
16182  - 1.51882 * cgagaHB
16183  + 5.46836 * dcZHB
16184  + 0.565585 * dKlambda
16185  + 0.000631004 * cZZHB * dKlambda
16186  - 0.195079 * cZgaHB * dKlambda
16187  + 0.064441 * cZboxHB * dKlambda
16188  + 0.440061 * cgagaHB * dKlambda
16189  + 2.13192 * dcZHB * dKlambda
16190  + 0.0968208 * dKlambda * dKlambda;
16191 
16192 // ILC report (1903.01629) gives total cross section a 4/ab: 16.8%.
16193 // Assume the precision for each polarization is the same as they do for single Higgs in ZH...
16194  Chi2p80m30 = Chi2p80m30 * Chi2p80m30 / 0.168 / 0.168 / 2.0;
16195 
16196 // The signal strength -1
16197  Chi2m80p30 = - 2.57112 * cZZHB
16198  + 6.97966 * cZgaHB
16199  - 10.2626 * cZboxHB
16200  + 1.39647 * cgagaHB
16201  + 5.4684 * dcZHB
16202  + 0.565577 * dKlambda
16203  + 4.71916 * cZZHB * dKlambda
16204  + 0.179045 * cZgaHB * dKlambda
16205  + 7.28766 * cZboxHB * dKlambda
16206  - 0.405166 * cgagaHB * dKlambda
16207  + 2.13189 * dcZHB * dKlambda
16208  + 0.0968201 * dKlambda * dKlambda;
16209 
16210 // ILC report (1903.01629) gives total cross section a 4/ab: 16.8%.
16211 // Assume the precision for each polarization is the same as they do for single Higgs in ZH...
16212  Chi2m80p30 = Chi2m80p30 * Chi2m80p30 / 0.168 / 0.168 / 2.0;
16213 
16214  Chi2Tot = Chi2p80m30 + Chi2m80p30;
16215 
16216  // To be used as Gaussian observable with mean=0, var=1 I must return the sqrt.
16217  return sqrt(Chi2Tot);
16218 }

◆ bPskPol()

double NPSMEFTd6::bPskPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(b_{eeZH}\)

Reimplemented from NPbase.

Definition at line 9022 of file NPSMEFTd6.cpp.

9023 {
9024  double bL, bR, bPol;
9025  double sM = sqrt_s * sqrt_s;
9026  double Mz2 = Mz*Mz;
9027 
9028  double ZetaZ, ZetaAZ;
9029  double CWB, CBB, CWW;
9030 
9031  // Convention for dim 6 operators
9033  CBB = 0.25 * (g2_tree*g2_tree/g1_tree/g1_tree) * CiHB * v2_over_LambdaNP2;
9034  CWW = 0.25 * CiHW * v2_over_LambdaNP2;
9035 
9036  ZetaZ = cW2_tree*8.0*CWW + 2.0*sW2_tree*8*CWB + (sW2_tree*sW2_tree/cW2_tree)*8.0*CBB;
9037  ZetaAZ = sW_tree*cW_tree*(8.0*CWW - (1.0 - sW2_tree/cW2_tree)*8*CWB - (sW2_tree/cW2_tree)*8.0*CBB);
9038 
9039  // LH and RH pars
9040  bL = ZetaZ + (sW_tree*cW_tree)/(0.5 - sW2_tree)*(sM - Mz2)/sM*ZetaAZ;
9041  bR = ZetaZ - (cW_tree/sW_tree)*(sM - Mz2)/sM*ZetaAZ;
9042 
9043  // Polarized b parameter
9044  bPol = 0.25 * ( (1.0 - Pol_em/100.0)*(1.0 + Pol_ep/100.0) * bL
9045  + (1.0 + Pol_em/100.0)*(1.0 - Pol_ep/100.0) * bR );
9046 
9047  return bPol;
9048 }

◆ Br_H_exo()

double NPSMEFTd6::Br_H_exo ( ) const
virtual

The branching ratio of the of the Higgs into exotic particles.

Returns
Br \((H\to exotic)\)

Reimplemented from NPbase.

Definition at line 12713 of file NPSMEFTd6.cpp.

12714 {
12715  if (BrHexo < 0) return std::numeric_limits<double>::quiet_NaN();
12716 
12717  return BrHexo;
12718 }

◆ Br_H_inv()

double NPSMEFTd6::Br_H_inv ( ) const
virtual

The branching ratio of the of the Higgs into invisible particles.

Returns
Br \((H\to invisible)\)

Reimplemented from NPbase.

Definition at line 12720 of file NPSMEFTd6.cpp.

12721 {
12722 // Contributions from both modifications in H->ZZ->4v and the extra invisible decays
12723  double BR4v;
12724 
12725  BR4v = BrHZZ4vRatio()*(trueSM.computeBrHtoZZinv());
12726 
12727 // BR4v positivity is already checked inside BrHZZ4vRatio()
12728 // and will be nan if negative. Check here BrHinv, to make sure both are positive
12729  if (BrHinv < 0) return std::numeric_limits<double>::quiet_NaN();
12730 
12731  return BR4v + BrHinv;
12732 }

◆ Br_H_inv_NP()

double NPSMEFTd6::Br_H_inv_NP ( ) const
virtual

The branching ratio of the of the Higgs into invisible particles (only invisible new particles).

Returns
Br \((H\to invisible,NP)\)

Reimplemented from NPbase.

Definition at line 12735 of file NPSMEFTd6.cpp.

12736 {
12737 
12738 // BR4v positivity is already checked inside BrHZZ4vRatio()
12739 // and will be nan if negative. Check here BrHinv, to make sure both are positive
12740  if (BrHinv < 0) return std::numeric_limits<double>::quiet_NaN();
12741 
12742  return BrHinv;
12743 }

◆ BrHbbRatio()

double NPSMEFTd6::BrHbbRatio ( ) const
virtual

The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.

Returns
Br \((H\to b\bar{b})\)/Br \((H\to b\bar{b})_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10866 of file NPSMEFTd6.cpp.

10867 {
10868  double Br = 1.0;
10869  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10870 
10871  dGHiR1= deltaGammaHbbRatio1();
10872 
10873  Br += dGHiR1 - dGammaHTotR1;
10874 
10875  if (FlagQuadraticTerms) {
10876 
10877  dGHiR2= deltaGammaHbbRatio2();
10878 
10879  //Add contributions that are quadratic in the effective coefficients
10880  Br += - dGHiR1 * dGammaHTotR1
10881  + dGHiR2 - dGammaHTotR2
10882  + pow(dGammaHTotR1,2.0);
10883  }
10884 
10885  GHiR += dGHiR1 + dGHiR2;
10886  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10887 
10888  return Br;
10889 
10890 }

◆ BrHccRatio()

double NPSMEFTd6::BrHccRatio ( ) const
virtual

The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.

Returns
Br \((H\to c\bar{c})\)/Br \((H\to c\bar{c})_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10840 of file NPSMEFTd6.cpp.

10841 {
10842  double Br = 1.0;
10843  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10844 
10845  dGHiR1= deltaGammaHccRatio1();
10846 
10847  Br += dGHiR1 - dGammaHTotR1;
10848 
10849  if (FlagQuadraticTerms) {
10850 
10851  dGHiR2= deltaGammaHccRatio2();
10852 
10853  //Add contributions that are quadratic in the effective coefficients
10854  Br += - dGHiR1 * dGammaHTotR1
10855  + dGHiR2 - dGammaHTotR2
10856  + pow(dGammaHTotR1,2.0);
10857  }
10858 
10859  GHiR += dGHiR1 + dGHiR2;
10860  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10861 
10862  return Br;
10863 
10864 }

◆ BrHgagaRatio()

double NPSMEFTd6::BrHgagaRatio ( ) const
virtual

The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to \gamma\gamma)\)/Br \((H\to \gamma\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10762 of file NPSMEFTd6.cpp.

10763 {
10764  double Br = 1.0;
10765  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10766 
10767  dGHiR1= deltaGammaHgagaRatio1();
10768 
10769  Br += dGHiR1 - dGammaHTotR1;
10770 
10771  if (FlagQuadraticTerms) {
10772 
10773  dGHiR2= deltaGammaHgagaRatio2();
10774 
10775  //Add contributions that are quadratic in the effective coefficients
10776  Br += - dGHiR1 * dGammaHTotR1
10777  + dGHiR2 - dGammaHTotR2
10778  + pow(dGammaHTotR1,2.0);
10779  }
10780 
10781  GHiR += dGHiR1 + dGHiR2;
10782  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10783 
10784  return Br;
10785 
10786 }

◆ BrHggRatio()

double NPSMEFTd6::BrHggRatio ( ) const
virtual

The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.

Returns
Br \((H\to gg)\)/Br \((H\to gg)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10202 of file NPSMEFTd6.cpp.

10203 {
10204  double Br = 1.0;
10205  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10206 
10207  dGHiR1= deltaGammaHggRatio1();
10208 
10209  Br += dGHiR1 - dGammaHTotR1;
10210 
10211  if (FlagQuadraticTerms) {
10212 
10213  dGHiR2= deltaGammaHggRatio2();
10214 
10215  //Add contributions that are quadratic in the effective coefficients
10216  Br += - dGHiR1 * dGammaHTotR1
10217  + dGHiR2 - dGammaHTotR2
10218  + pow(dGammaHTotR1,2.0);
10219  }
10220 
10221  GHiR += dGHiR1 + dGHiR2;
10222  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10223 
10224  return Br;
10225 
10226 }

◆ BrHmumuRatio()

double NPSMEFTd6::BrHmumuRatio ( ) const
virtual

The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.

Returns
Br \((H\to \mu^+\mu^-)\)/Br \((H\to \mu^+\mu^-)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10788 of file NPSMEFTd6.cpp.

10789 {
10790  double Br = 1.0;
10791  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10792 
10793  dGHiR1= deltaGammaHmumuRatio1();
10794 
10795  Br += dGHiR1 - dGammaHTotR1;
10796 
10797  if (FlagQuadraticTerms) {
10798 
10799  dGHiR2= deltaGammaHmumuRatio2();
10800 
10801  //Add contributions that are quadratic in the effective coefficients
10802  Br += - dGHiR1 * dGammaHTotR1
10803  + dGHiR2 - dGammaHTotR2
10804  + pow(dGammaHTotR1,2.0);
10805  }
10806 
10807  GHiR += dGHiR1 + dGHiR2;
10808  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10809 
10810  return Br;
10811 
10812 }

◆ BrHtautauRatio()

double NPSMEFTd6::BrHtautauRatio ( ) const
virtual

The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.

Returns
Br \((H\to \tau^+\tau^-)\)/Br \((H\to \tau^+\tau^-)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10814 of file NPSMEFTd6.cpp.

10815 {
10816  double Br = 1.0;
10817  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10818 
10819  dGHiR1= deltaGammaHtautauRatio1();
10820 
10821  Br += dGHiR1 - dGammaHTotR1;
10822 
10823  if (FlagQuadraticTerms) {
10824 
10825  dGHiR2= deltaGammaHtautauRatio2();
10826 
10827  //Add contributions that are quadratic in the effective coefficients
10828  Br += - dGHiR1 * dGammaHTotR1
10829  + dGHiR2 - dGammaHTotR2
10830  + pow(dGammaHTotR1,2.0);
10831  }
10832 
10833  GHiR += dGHiR1 + dGHiR2;
10834  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10835 
10836  return Br;
10837 
10838 }

◆ BrHtoinvRatio()

double NPSMEFTd6::BrHtoinvRatio ( ) const
virtual

The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.

Returns
Br \((H\to invisible)\)/Br \((H\to ZZ \to invisible)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 12794 of file NPSMEFTd6.cpp.

12795 {
12796  return (Br_H_inv()/(trueSM.computeBrHtoZZinv()));
12797 }

◆ BrHvisRatio()

double NPSMEFTd6::BrHvisRatio ( ) const
virtual

The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.

Returns
Br \((H\to visible)\)/Br \((H\to visible)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 12746 of file NPSMEFTd6.cpp.

12747 {
12748  double Br = 1.0;
12749  double dvis1 = 0.0, dvis2 = 0.0, delta2SM;
12750  double GHvisR = 1.0;
12751 
12752 // Sum over decays of visible SM and exotic modes
12762  + BrHexo);
12763 
12764  Br += dvis1 - dGammaHTotR1;
12765 
12766  if (FlagQuadraticTerms) {
12767 
12768 // Sum over decays of visible SM and exotic modes
12769  delta2SM = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
12778 
12779  dvis2 = delta2SM + (BrHexo)*(BrHexo + delta2SM);
12780 
12781  //Add contributions that are quadratic in the effective coefficients
12782  Br += - dvis1 * dGammaHTotR1
12783  + dvis2 - dGammaHTotR2
12784  + pow(dGammaHTotR1,2.0);
12785  }
12786 
12787  GHvisR += dvis1 + dvis2;
12788  if ((Br < 0) || (GHvisR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
12789 
12790  return Br;
12791 }

◆ BrHWffRatio()

double NPSMEFTd6::BrHWffRatio ( ) const
virtual

The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to W f f)\)/Br \((H\to W f f)_{\mathrm{SM}}\)

Definition at line 10335 of file NPSMEFTd6.cpp.

10336 {
10337  double Br = 1.0;
10338  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10339 
10340  dGHiR1= deltaGammaHWffRatio1();
10341 
10342  Br += dGHiR1 - dGammaHTotR1;
10343 
10344  if (FlagQuadraticTerms) {
10345 
10346  dGHiR2= deltaGammaHWffRatio2();
10347 
10348  //Add contributions that are quadratic in the effective coefficients
10349  Br += - dGHiR1 * dGammaHTotR1
10350  + dGHiR2 - dGammaHTotR2
10351  + pow(dGammaHTotR1,2.0);
10352  }
10353 
10354  GHiR += dGHiR1 + dGHiR2;
10355  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10356 
10357  return Br;
10358 }

◆ BrHWjjRatio()

double NPSMEFTd6::BrHWjjRatio ( ) const
virtual

The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model.

Returns
Br \((H\to W j j)\)/Br \((H\to W j j)_{\mathrm{SM}}\)

Definition at line 10285 of file NPSMEFTd6.cpp.

10286 {
10287  double Br = 1.0;
10288  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10289 
10290  dGHiR1= deltaGammaHWjjRatio1();
10291 
10292  Br += dGHiR1 - dGammaHTotR1;
10293 
10294  if (FlagQuadraticTerms) {
10295 
10296  dGHiR2= deltaGammaHWjjRatio2();
10297 
10298  //Add contributions that are quadratic in the effective coefficients
10299  Br += - dGHiR1 * dGammaHTotR1
10300  + dGHiR2 - dGammaHTotR2
10301  + pow(dGammaHTotR1,2.0);
10302  }
10303 
10304  GHiR += dGHiR1 + dGHiR2;
10305  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10306 
10307  return Br;
10308 }

◆ BrHWlvRatio()

double NPSMEFTd6::BrHWlvRatio ( ) const
virtual

The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Wl\nu)\)/Br \((H\to Wl\nu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10235 of file NPSMEFTd6.cpp.

10236 {
10237  double Br = 1.0;
10238  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10239 
10240  dGHiR1= deltaGammaHWlvRatio1();
10241 
10242  Br += dGHiR1 - dGammaHTotR1;
10243 
10244  if (FlagQuadraticTerms) {
10245 
10246  dGHiR2= deltaGammaHWlvRatio2();
10247 
10248  //Add contributions that are quadratic in the effective coefficients
10249  Br += - dGHiR1 * dGammaHTotR1
10250  + dGHiR2 - dGammaHTotR2
10251  + pow(dGammaHTotR1,2.0);
10252  }
10253 
10254  GHiR += dGHiR1 + dGHiR2;
10255  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10256 
10257  return Br;
10258 }

◆ BrHWW2l2vRatio()

double NPSMEFTd6::BrHWW2l2vRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to l\nu l\nu)\)/Br \((H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10260 of file NPSMEFTd6.cpp.

10261 {
10262  double Br = 1.0;
10263  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10264 
10265  dGHiR1= deltaGammaHWW2l2vRatio1();
10266 
10267  Br += dGHiR1 - dGammaHTotR1;
10268 
10269  if (FlagQuadraticTerms) {
10270 
10271  dGHiR2= deltaGammaHWW2l2vRatio2();
10272 
10273  //Add contributions that are quadratic in the effective coefficients
10274  Br += - dGHiR1 * dGammaHTotR1
10275  + dGHiR2 - dGammaHTotR2
10276  + pow(dGammaHTotR1,2.0);
10277  }
10278 
10279  GHiR += dGHiR1 + dGHiR2;
10280  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10281 
10282  return Br;
10283 }

◆ BrHWW4fRatio()

double NPSMEFTd6::BrHWW4fRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to 4f)\)/Br \((H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 10361 of file NPSMEFTd6.cpp.

10362 {
10363  double Br = 1.0;
10364  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10365 
10366  dGHiR1= deltaGammaHWW4fRatio1();
10367 
10368  Br += dGHiR1 - dGammaHTotR1;
10369 
10370  if (FlagQuadraticTerms) {
10371 
10372  dGHiR2= deltaGammaHWW4fRatio2();
10373 
10374  //Add contributions that are quadratic in the effective coefficients
10375  Br += - dGHiR1 * dGammaHTotR1
10376  + dGHiR2 - dGammaHTotR2
10377  + pow(dGammaHTotR1,2.0);
10378  }
10379 
10380  GHiR += dGHiR1 + dGHiR2;
10381  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10382 
10383  return Br;
10384 }

◆ BrHWW4jRatio()

double NPSMEFTd6::BrHWW4jRatio ( ) const
virtual

The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model.

Returns
Br \((H\to WW^*\to 4j)\)/Br \((H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 10310 of file NPSMEFTd6.cpp.

10311 {
10312  double Br = 1.0;
10313  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10314 
10315  dGHiR1= deltaGammaHWW4jRatio1();
10316 
10317  Br += dGHiR1 - dGammaHTotR1;
10318 
10319  if (FlagQuadraticTerms) {
10320 
10321  dGHiR2= deltaGammaHWW4jRatio2();
10322 
10323  //Add contributions that are quadratic in the effective coefficients
10324  Br += - dGHiR1 * dGammaHTotR1
10325  + dGHiR2 - dGammaHTotR2
10326  + pow(dGammaHTotR1,2.0);
10327  }
10328 
10329  GHiR += dGHiR1 + dGHiR2;
10330  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10331 
10332  return Br;
10333 }

◆ BrHWWRatio()

double NPSMEFTd6::BrHWWRatio ( ) const
virtual

The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.

Returns
Br \((H\to WW)\)/Br \((H\to WW)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10228 of file NPSMEFTd6.cpp.

10229 {
10230 
10231  return BrHWW4fRatio();
10232 
10233 }

◆ BrHZddRatio()

double NPSMEFTd6::BrHZddRatio ( ) const
virtual

The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z d d)\)/Br \((H\to Z d d)_{\mathrm{SM}}\)

Definition at line 10606 of file NPSMEFTd6.cpp.

10607 {
10608  double Br = 1.0;
10609  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10610 
10611  dGHiR1= deltaGammaHZddRatio1();
10612 
10613  Br += dGHiR1 - dGammaHTotR1;
10614 
10615  if (FlagQuadraticTerms) {
10616 
10617  dGHiR2= deltaGammaHZddRatio2();
10618 
10619  //Add contributions that are quadratic in the effective coefficients
10620  Br += - dGHiR1 * dGammaHTotR1
10621  + dGHiR2 - dGammaHTotR2
10622  + pow(dGammaHTotR1,2.0);
10623  }
10624 
10625  GHiR += dGHiR1 + dGHiR2;
10626  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10627 
10628  return Br;
10629 }

◆ BrHZffRatio()

double NPSMEFTd6::BrHZffRatio ( ) const
virtual

The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to Zff)\)/Br \((H\to Zff)_{\mathrm{SM}}\)

Definition at line 10649 of file NPSMEFTd6.cpp.

10650 {
10651  double Br = 1.0;
10652  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10653 
10654  dGHiR1= deltaGammaHZffRatio1();
10655 
10656  Br += dGHiR1 - dGammaHTotR1;
10657 
10658  if (FlagQuadraticTerms) {
10659 
10660  dGHiR2= deltaGammaHZffRatio2();
10661 
10662  //Add contributions that are quadratic in the effective coefficients
10663  Br += - dGHiR1 * dGammaHTotR1
10664  + dGHiR2 - dGammaHTotR2
10665  + pow(dGammaHTotR1,2.0);
10666  }
10667 
10668  GHiR += dGHiR1 + dGHiR2;
10669  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10670 
10671  return Br;
10672 }

◆ BrHZgaeeRatio()

double NPSMEFTd6::BrHZgaeeRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to ee\gamma)\)/Br \((H\to Z\gamma\to ee\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10740 of file NPSMEFTd6.cpp.

10741 {
10742  double deltaBRratio;
10743 
10744  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON]) / (trueSM.GammaZ(leptons[ELECTRON]));
10745 
10746  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10747 
10748  return ( BrHZgaRatio() + deltaBRratio );
10749 }

◆ BrHZgallRatio()

double NPSMEFTd6::BrHZgallRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to ll\gamma)\)/Br \((H\to Z\gamma\to ll\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10725 of file NPSMEFTd6.cpp.

10726 {
10727  double deltaBRratio;
10728 
10729  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
10730  + deltaGamma_Zf(leptons[MU]);
10731 
10732  deltaBRratio = deltaBRratio /
10734 
10735  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10736 
10737  return ( BrHZgaRatio() + deltaBRratio );
10738 }

◆ BrHZgamumuRatio()

double NPSMEFTd6::BrHZgamumuRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma\to \mu\mu\gamma)\)/Br \((H\to Z\gamma\to \mu\mu\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10751 of file NPSMEFTd6.cpp.

10752 {
10753  double deltaBRratio;
10754 
10755  deltaBRratio = deltaGamma_Zf(leptons[MU])/(trueSM.GammaZ(leptons[MU]));
10756 
10757  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10758 
10759  return ( BrHZgaRatio() + deltaBRratio );
10760 }

◆ BrHZgaRatio()

double NPSMEFTd6::BrHZgaRatio ( ) const
virtual

The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\gamma)\)/Br \((H\to Z\gamma)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10699 of file NPSMEFTd6.cpp.

10700 {
10701  double Br = 1.0;
10702  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10703 
10704  dGHiR1= deltaGammaHZgaRatio1();
10705 
10706  Br += dGHiR1 - dGammaHTotR1;
10707 
10708  if (FlagQuadraticTerms) {
10709 
10710  dGHiR2= deltaGammaHZgaRatio2();
10711 
10712  //Add contributions that are quadratic in the effective coefficients
10713  Br += - dGHiR1 * dGammaHTotR1
10714  + dGHiR2 - dGammaHTotR2
10715  + pow(dGammaHTotR1,2.0);
10716  }
10717 
10718  GHiR += dGHiR1 + dGHiR2;
10719  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10720 
10721  return Br;
10722 
10723 }

◆ BrHZllRatio()

double NPSMEFTd6::BrHZllRatio ( ) const
virtual

The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to Zll)\)/Br \((H\to Zll)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10391 of file NPSMEFTd6.cpp.

10392 {
10393  double Br = 1.0;
10394  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10395 
10396  dGHiR1= deltaGammaHZllRatio1();
10397 
10398  Br += dGHiR1 - dGammaHTotR1;
10399 
10400  if (FlagQuadraticTerms) {
10401 
10402  dGHiR2= deltaGammaHZllRatio2();
10403 
10404  //Add contributions that are quadratic in the effective coefficients
10405  Br += - dGHiR1 * dGammaHTotR1
10406  + dGHiR2 - dGammaHTotR2
10407  + pow(dGammaHTotR1,2.0);
10408  }
10409 
10410  GHiR += dGHiR1 + dGHiR2;
10411  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10412 
10413  return Br;
10414 }

◆ BrHZuuRatio()

double NPSMEFTd6::BrHZuuRatio ( ) const
virtual

The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
Br \((H\to Z u u)\)/Br \((H\to Z u u)_{\mathrm{SM}}\)

Definition at line 10566 of file NPSMEFTd6.cpp.

10567 {
10568  double Br = 1.0;
10569  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10570 
10571  dGHiR1= deltaGammaHZuuRatio1();
10572 
10573  Br += dGHiR1 - dGammaHTotR1;
10574 
10575  if (FlagQuadraticTerms) {
10576 
10577  dGHiR2= deltaGammaHZuuRatio2();
10578 
10579  //Add contributions that are quadratic in the effective coefficients
10580  Br += - dGHiR1 * dGammaHTotR1
10581  + dGHiR2 - dGammaHTotR2
10582  + pow(dGammaHTotR1,2.0);
10583  }
10584 
10585  GHiR += dGHiR1 + dGHiR2;
10586  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10587 
10588  return Br;
10589 }

◆ BrHZvvRatio()

double NPSMEFTd6::BrHZvvRatio ( ) const
virtual

The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model.

Returns
Br \((H\to Z\nu\nu)\)/Br \((H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 10516 of file NPSMEFTd6.cpp.

10517 {
10518  double Br = 1.0;
10519  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10520 
10521  dGHiR1= deltaGammaHZvvRatio1();
10522 
10523  Br += dGHiR1 - dGammaHTotR1;
10524 
10525  if (FlagQuadraticTerms) {
10526 
10527  dGHiR2= deltaGammaHZvvRatio2();
10528 
10529  //Add contributions that are quadratic in the effective coefficients
10530  Br += - dGHiR1 * dGammaHTotR1
10531  + dGHiR2 - dGammaHTotR2
10532  + pow(dGammaHTotR1,2.0);
10533  }
10534 
10535  GHiR += dGHiR1 + dGHiR2;
10536  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10537 
10538  return Br;
10539 }

◆ BrHZZ2e2muRatio()

double NPSMEFTd6::BrHZZ2e2muRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 2e 2\mu)\)/Br \((H\to ZZ* \to 2e 2\mu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10466 of file NPSMEFTd6.cpp.

10467 {
10468  double Br = 1.0;
10469  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10470 
10471  dGHiR1= deltaGammaHZZ2e2muRatio1();
10472 
10473  Br += dGHiR1 - dGammaHTotR1;
10474 
10475  if (FlagQuadraticTerms) {
10476 
10477  dGHiR2= deltaGammaHZZ2e2muRatio2();
10478 
10479  //Add contributions that are quadratic in the effective coefficients
10480  Br += - dGHiR1 * dGammaHTotR1
10481  + dGHiR2 - dGammaHTotR2
10482  + pow(dGammaHTotR1,2.0);
10483  }
10484 
10485  GHiR += dGHiR1 + dGHiR2;
10486  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10487 
10488  return Br;
10489 }

◆ BrHZZ4dRatio()

double NPSMEFTd6::BrHZZ4dRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4 d)\)/Br \((H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 10631 of file NPSMEFTd6.cpp.

10632 {
10633  double deltaBRratio;
10634 
10635  deltaBRratio = deltaGamma_Zf(quarks[DOWN])
10638 
10639  deltaBRratio = deltaBRratio /
10640  ( trueSM.GammaZ(quarks[DOWN])
10642  + trueSM.GammaZ(quarks[BOTTOM]) );
10643 
10644  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10645 
10646  return ( BrHZddRatio() + deltaBRratio );
10647 }

◆ BrHZZ4eRatio()

double NPSMEFTd6::BrHZZ4eRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4e)\)/Br \((H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10441 of file NPSMEFTd6.cpp.

10442 {
10443  double Br = 1.0;
10444  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10445 
10446  dGHiR1= deltaGammaHZZ4eRatio1();
10447 
10448  Br += dGHiR1 - dGammaHTotR1;
10449 
10450  if (FlagQuadraticTerms) {
10451 
10452  dGHiR2= deltaGammaHZZ4eRatio2();
10453 
10454  //Add contributions that are quadratic in the effective coefficients
10455  Br += - dGHiR1 * dGammaHTotR1
10456  + dGHiR2 - dGammaHTotR2
10457  + pow(dGammaHTotR1,2.0);
10458  }
10459 
10460  GHiR += dGHiR1 + dGHiR2;
10461  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10462 
10463  return Br;
10464 }

◆ BrHZZ4fRatio()

double NPSMEFTd6::BrHZZ4fRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4f)\)/Br \((H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 10674 of file NPSMEFTd6.cpp.

10675 {
10676  double Br = 1.0;
10677  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10678 
10679  dGHiR1= deltaGammaHZZ4fRatio1();
10680 
10681  Br += dGHiR1 - dGammaHTotR1;
10682 
10683  if (FlagQuadraticTerms) {
10684 
10685  dGHiR2= deltaGammaHZZ4fRatio2();
10686 
10687  //Add contributions that are quadratic in the effective coefficients
10688  Br += - dGHiR1 * dGammaHTotR1
10689  + dGHiR2 - dGammaHTotR2
10690  + pow(dGammaHTotR1,2.0);
10691  }
10692 
10693  GHiR += dGHiR1 + dGHiR2;
10694  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10695 
10696  return Br;
10697 }

◆ BrHZZ4lRatio()

double NPSMEFTd6::BrHZZ4lRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4l)\)/Br \((H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10416 of file NPSMEFTd6.cpp.

10417 {
10418  double Br = 1.0;
10419  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10420 
10421  dGHiR1= deltaGammaHZZ4lRatio1();
10422 
10423  Br += dGHiR1 - dGammaHTotR1;
10424 
10425  if (FlagQuadraticTerms) {
10426 
10427  dGHiR2= deltaGammaHZZ4lRatio2();
10428 
10429  //Add contributions that are quadratic in the effective coefficients
10430  Br += - dGHiR1 * dGammaHTotR1
10431  + dGHiR2 - dGammaHTotR2
10432  + pow(dGammaHTotR1,2.0);
10433  }
10434 
10435  GHiR += dGHiR1 + dGHiR2;
10436  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10437 
10438  return Br;
10439 }

◆ BrHZZ4muRatio()

double NPSMEFTd6::BrHZZ4muRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4\mu)\)/Br \((H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10491 of file NPSMEFTd6.cpp.

10492 {
10493  double Br = 1.0;
10494  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10495 
10496  dGHiR1= deltaGammaHZZ4muRatio1();
10497 
10498  Br += dGHiR1 - dGammaHTotR1;
10499 
10500  if (FlagQuadraticTerms) {
10501 
10502  dGHiR2= deltaGammaHZZ4muRatio2();
10503 
10504  //Add contributions that are quadratic in the effective coefficients
10505  Br += - dGHiR1 * dGammaHTotR1
10506  + dGHiR2 - dGammaHTotR2
10507  + pow(dGammaHTotR1,2.0);
10508  }
10509 
10510  GHiR += dGHiR1 + dGHiR2;
10511  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10512 
10513  return Br;
10514 }

◆ BrHZZ4uRatio()

double NPSMEFTd6::BrHZZ4uRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4 u)\)/Br \((H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

Definition at line 10591 of file NPSMEFTd6.cpp.

10592 {
10593  double deltaBRratio;
10594 
10595  deltaBRratio = deltaGamma_Zf(quarks[UP])
10597 
10598  deltaBRratio = deltaBRratio /
10600 
10601  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
10602 
10603  return ( BrHZuuRatio() + deltaBRratio );
10604 }

◆ BrHZZ4vRatio()

double NPSMEFTd6::BrHZZ4vRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ* \to 4\nu)\)/Br \((H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 10541 of file NPSMEFTd6.cpp.

10542 {
10543  double Br = 1.0;
10544  double dGHiR1=0.0, dGHiR2=0.0, GHiR=1.0;
10545 
10546  dGHiR1= deltaGammaHZZ4vRatio1();
10547 
10548  Br += dGHiR1 - dGammaHTotR1;
10549 
10550  if (FlagQuadraticTerms) {
10551 
10552  dGHiR2= deltaGammaHZZ4vRatio2();
10553 
10554  //Add contributions that are quadratic in the effective coefficients
10555  Br += - dGHiR1 * dGammaHTotR1
10556  + dGHiR2 - dGammaHTotR2
10557  + pow(dGammaHTotR1,2.0);
10558  }
10559 
10560  GHiR += dGHiR1 + dGHiR2;
10561  if ((Br < 0) || (GHiR < 0) || (GammaHTotR < 0)) return std::numeric_limits<double>::quiet_NaN();
10562 
10563  return Br;
10564 }

◆ BrHZZRatio()

double NPSMEFTd6::BrHZZRatio ( ) const
virtual

The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.

Returns
Br \((H\to ZZ)\)/Br \((H\to ZZ)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10386 of file NPSMEFTd6.cpp.

10387 {
10388  return BrHZZ4fRatio();
10389 }

◆ CfB_diag()

gslpp::complex NPSMEFTd6::CfB_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fB})_{ff} \(\)

Definition at line 2893 of file NPSMEFTd6.cpp.

2894 {
2895  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2896  return 0.0;
2897  else if (f.is("ELECTRON"))
2898  return 0.0;
2899  else if (f.is("MU"))
2900  return 0.0;
2901  else if (f.is("TAU"))
2902  return 0.0;
2903  else if (f.is("UP"))
2904  return gslpp::complex(CiuB_11r, CuB_11i, false);
2905  else if (f.is("CHARM"))
2906  return gslpp::complex(CiuB_22r, CuB_22i, false);
2907  else if (f.is("TOP"))
2908  return gslpp::complex(CiuB_33r, CuB_33i, false);
2909  else if (f.is("DOWN"))
2910  return 0.0;
2911  else if (f.is("STRANGE"))
2912  return 0.0;
2913  else if (f.is("BOTTOM"))
2914  return 0.0;
2915  else
2916  throw std::runtime_error("NPSMEFTd6::CfB_diag(): wrong argument");
2917 }

◆ CfG_diag()

gslpp::complex NPSMEFTd6::CfG_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fG})_{ff} \(\)

Definition at line 2841 of file NPSMEFTd6.cpp.

2842 {
2843  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2844  return 0.0;
2845  else if (f.is("ELECTRON"))
2846  return 0.0;
2847  else if (f.is("MU"))
2848  return 0.0;
2849  else if (f.is("TAU"))
2850  return 0.0;
2851  else if (f.is("UP"))
2852  return gslpp::complex(CiuG_11r, CuG_11i, false);
2853  else if (f.is("CHARM"))
2854  return gslpp::complex(CiuG_22r, CuG_22i, false);
2855  else if (f.is("TOP"))
2856  return gslpp::complex(CiuG_33r, CuG_33i, false);
2857  else if (f.is("DOWN"))
2858  return 0.0;
2859  else if (f.is("STRANGE"))
2860  return 0.0;
2861  else if (f.is("BOTTOM"))
2862  return 0.0;
2863  else
2864  throw std::runtime_error("NPSMEFTd6::CfG_diag(): wrong argument");
2865 }

◆ CfH_diag()

gslpp::complex NPSMEFTd6::CfH_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fH})_{ff} \(\)

Definition at line 2815 of file NPSMEFTd6.cpp.

2816 {
2817  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2818  return 0.0;
2819  else if (f.is("ELECTRON"))
2820  return gslpp::complex(CieH_11r, CeH_11i, false);
2821  else if (f.is("MU"))
2822  return gslpp::complex(CieH_22r, CeH_22i, false);
2823  else if (f.is("TAU"))
2824  return gslpp::complex(CieH_33r, CeH_33i, false);
2825  else if (f.is("UP"))
2826  return gslpp::complex(CiuH_11r, CuH_11i, false);
2827  else if (f.is("CHARM"))
2828  return gslpp::complex(CiuH_22r, CuH_22i, false);
2829  else if (f.is("TOP"))
2830  return gslpp::complex(CiuH_33r, CuH_33i, false);
2831  else if (f.is("DOWN"))
2832  return gslpp::complex(CidH_11r, CdH_11i, false);
2833  else if (f.is("STRANGE"))
2834  return gslpp::complex(CidH_22r, CdH_22i, false);
2835  else if (f.is("BOTTOM"))
2836  return gslpp::complex(CidH_33r, CdH_33i, false);
2837  else
2838  throw std::runtime_error("NPSMEFTd6::CfH_diag(): wrong argument");
2839 }

◆ CfW_diag()

gslpp::complex NPSMEFTd6::CfW_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{fW})_{ff} \(\)

Definition at line 2867 of file NPSMEFTd6.cpp.

2868 {
2869  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2870  return 0.0;
2871  else if (f.is("ELECTRON"))
2872  return 0.0;
2873  else if (f.is("MU"))
2874  return 0.0;
2875  else if (f.is("TAU"))
2876  return 0.0;
2877  else if (f.is("UP"))
2878  return gslpp::complex(CiuW_11r, CuW_11i, false);
2879  else if (f.is("CHARM"))
2880  return gslpp::complex(CiuW_22r, CuW_22i, false);
2881  else if (f.is("TOP"))
2882  return gslpp::complex(CiuW_33r, CuW_33i, false);
2883  else if (f.is("DOWN"))
2884  return 0.0;
2885  else if (f.is("STRANGE"))
2886  return 0.0;
2887  else if (f.is("BOTTOM"))
2888  return 0.0;
2889  else
2890  throw std::runtime_error("NPSMEFTd6::CfW_diag(): wrong argument");
2891 }

◆ cgaga_HB()

double NPSMEFTd6::cgaga_HB ( ) const
virtual

The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 15570 of file NPSMEFTd6.cpp.

15571 {
15572  double ciHB;
15573 
15575 
15576  return ciHB;
15577 }

◆ cgg_HB()

double NPSMEFTd6::cgg_HB ( ) const
virtual

The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{gg}\)

Reimplemented from NPbase.

Definition at line 15580 of file NPSMEFTd6.cpp.

15581 {
15582  double ciHB;
15583 
15584  ciHB = (1.0/(M_PI * AlsMz))*CHG*v2_over_LambdaNP2;
15585 
15586  return ciHB;
15587 }

◆ cggEff_HB()

double NPSMEFTd6::cggEff_HB ( ) const
virtual

The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{gg}^{Eff}\)

Reimplemented from NPbase.

Definition at line 15589 of file NPSMEFTd6.cpp.

15590 {
15591  double ciHB;
15592 
15593  double m_t = mtpole;
15594  //doulbe m_t = quarks[TOP].getMass();
15595  double m_b = quarks[BOTTOM].getMass();
15596  double m_c = quarks[CHARM].getMass();
15597 
15598  double At = deltayt_HB() * AH_f(4.0 * m_t * m_t / mHl / mHl).real();
15599  double Ab = deltayb_HB() * AH_f(4.0 * m_b * m_b / mHl / mHl).real();
15600  double Ac = deltayc_HB() * AH_f(4.0 * m_c * m_c / mHl / mHl).real();
15601 
15602  ciHB = cgg_HB() + (1.0/16.0/M_PI/M_PI) * (At + Ab + Ac) ;
15603 
15604  return ciHB;
15605 }

◆ CheckParameters()

bool NPSMEFTd6::CheckParameters ( const std::map< std::string, double > &  DPars)
virtual

A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization.

Parameters
[in]DParsa map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant)
Returns
a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 2652 of file NPSMEFTd6.cpp.

2653 {
2655  if (FlagRotateCHWCHB) {
2656  for (int i = 0; i < NNPSMEFTd6Vars_LFU_QFU; i++) {
2657  if (DPars.find(NPSMEFTd6VarsRot_LFU_QFU[i]) == DPars.end()) {
2658  std::cout << "ERROR: Missing mandatory NPSMEFTd6_LFU_QFU parameter "
2659  << NPSMEFTd6VarsRot_LFU_QFU[i] << std::endl;
2662  }
2663  }
2664  } else {
2665  for (int i = 0; i < NNPSMEFTd6Vars_LFU_QFU; i++) {
2666  if (DPars.find(NPSMEFTd6Vars_LFU_QFU[i]) == DPars.end()) {
2667  std::cout << "ERROR: Missing mandatory NPSMEFTd6_LFU_QFU parameter "
2668  << NPSMEFTd6Vars_LFU_QFU[i] << std::endl;
2671  }
2672  }
2673  }
2674  } else if (!FlagLeptonUniversal && !FlagQuarkUniversal) {
2675  if (FlagRotateCHWCHB) {
2676  for (int i = 0; i < NNPSMEFTd6Vars; i++) {
2677  if (DPars.find(NPSMEFTd6VarsRot[i]) == DPars.end()) {
2678  std::cout << "ERROR: Missing mandatory NPSMEFTd6 parameter "
2679  << NPSMEFTd6VarsRot[i] << std::endl;
2682  }
2683  }
2684  } else {
2685  for (int i = 0; i < NNPSMEFTd6Vars; i++) {
2686  if (DPars.find(NPSMEFTd6Vars[i]) == DPars.end()) {
2687  std::cout << "ERROR: Missing mandatory NPSMEFTd6 parameter "
2688  << NPSMEFTd6Vars[i] << std::endl;
2691  }
2692  }
2693  }
2694 
2695  } else
2696  throw std::runtime_error("Error in NPSMEFTd6::CheckParameters()");
2697 
2698  return (NPbase::CheckParameters(DPars));
2699 }

◆ CHF1_diag()

double NPSMEFTd6::CHF1_diag ( const Particle  F) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.

Parameters
[in]Fa lepton or quark
Returns
\((\)C_{HF}^{(1)})_{FF} \(\)

Definition at line 2738 of file NPSMEFTd6.cpp.

2739 {
2740  if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
2741  return CiHL1_11;
2742  else if (F.is("NEUTRINO_2") || F.is("MU"))
2743  return CiHL1_22;
2744  else if (F.is("NEUTRINO_3") || F.is("TAU"))
2745  return CiHL1_33;
2746  else if (F.is("UP") || F.is("DOWN"))
2747  return CiHQ1_11;
2748  else if (F.is("CHARM") || F.is("STRANGE"))
2749  return CiHQ1_22;
2750  else if (F.is("TOP") || F.is("BOTTOM"))
2751  return CiHQ1_33;
2752  else
2753  throw std::runtime_error("NPSMEFTd6::CHF1_diag(): wrong argument");
2754 }

◆ CHF3_diag()

double NPSMEFTd6::CHF3_diag ( const Particle  F) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.

Parameters
[in]Fa lepton or quark
Returns
\((\)C_{HF}^{(3)})_{FF} \(\)

Definition at line 2756 of file NPSMEFTd6.cpp.

2757 {
2758  if (F.is("NEUTRINO_1") || F.is("ELECTRON"))
2759  return CiHL3_11;
2760  else if (F.is("NEUTRINO_2") || F.is("MU"))
2761  return CiHL3_22;
2762  else if (F.is("NEUTRINO_3") || F.is("TAU"))
2763  return CiHL3_33;
2764  else if (F.is("UP") || F.is("DOWN"))
2765  return CiHQ3_11;
2766  else if (F.is("CHARM") || F.is("STRANGE"))
2767  return CiHQ3_22;
2768  else if (F.is("TOP") || F.is("BOTTOM"))
2769  return CiHQ3_33;
2770  else
2771  throw std::runtime_error("NPSMEFTd6::CHF3_diag(): wrong argument");
2772 }

◆ CHf_diag()

double NPSMEFTd6::CHf_diag ( const Particle  f) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.

Parameters
[in]fa lepton or quark
Returns
\((\)C_{Hf})_{ff} \(\)

Definition at line 2774 of file NPSMEFTd6.cpp.

2775 {
2776  if (f.is("NEUTRINO_1") || f.is("NEUTRINO_2") || f.is("NEUTRINO_3"))
2777  return 0.0;
2778  else if (f.is("ELECTRON"))
2779  return CiHe_11;
2780  else if (f.is("MU"))
2781  return CiHe_22;
2782  else if (f.is("TAU"))
2783  return CiHe_33;
2784  else if (f.is("UP"))
2785  return CiHu_11;
2786  else if (f.is("CHARM"))
2787  return CiHu_22;
2788  else if (f.is("TOP"))
2789  return CiHu_33;
2790  else if (f.is("DOWN"))
2791  return CiHd_11;
2792  else if (f.is("STRANGE"))
2793  return CiHd_22;
2794  else if (f.is("BOTTOM"))
2795  return CiHd_33;
2796  else
2797  throw std::runtime_error("NPSMEFTd6::CHf_diag(): wrong argument");
2798 }

◆ CHud_diag()

gslpp::complex NPSMEFTd6::CHud_diag ( const Particle  u) const
protected

The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f.

Parameters
[in]ua quark
Returns
\((\)C_{Hud})_{ud} \(\)

Definition at line 2800 of file NPSMEFTd6.cpp.

2801 {
2802  if (!u.is("QUARK") || u.getIndex() % 2 != 0)
2803  throw std::runtime_error("NPSMEFTd6::CHud_diag(): wrong argument");
2804 
2805  if (u.is("UP"))
2806  return gslpp::complex(CHud_11r, CHud_11i, false);
2807  else if (u.is("CHARM"))
2808  return gslpp::complex(CHud_22r, CHud_22i, false);
2809  else if (u.is("TOP"))
2810  return gslpp::complex(CHud_22r, CHud_33i, false);
2811  else
2812  throw std::runtime_error("NPSMEFTd6::CHud_diag(): wrong argument");
2813 }

◆ CLL_bottom()

double NPSMEFTd6::CLL_bottom ( ) const

Definition at line 16494 of file NPSMEFTd6.cpp.

16495 {
16497 }

◆ CLL_charm()

double NPSMEFTd6::CLL_charm ( ) const

Definition at line 16484 of file NPSMEFTd6.cpp.

16485 {
16487 }

◆ CLL_down()

double NPSMEFTd6::CLL_down ( ) const

Definition at line 16479 of file NPSMEFTd6.cpp.

16480 {
16481  return (CLQ1_1111+CLQ3_1111);
16482 }

◆ CLL_mu()

double NPSMEFTd6::CLL_mu ( ) const

Definition at line 16464 of file NPSMEFTd6.cpp.

16465 {
16466  return (CLL_1122 + CLL_2211 + CiLL_1221 + CiLL_2112);
16467 }

◆ CLL_strange()

double NPSMEFTd6::CLL_strange ( ) const

Definition at line 16489 of file NPSMEFTd6.cpp.

16490 {
16492 }

◆ CLL_tau()

double NPSMEFTd6::CLL_tau ( ) const

Definition at line 16469 of file NPSMEFTd6.cpp.

16470 {
16471  return (CLL_1133 + CLL_3311 + CLL_1331 + CLL_3113);
16472 }

◆ CLL_up()

double NPSMEFTd6::CLL_up ( ) const

Definition at line 16474 of file NPSMEFTd6.cpp.

16475 {
16476  return (CLQ1_1111-CLQ3_1111);
16477 }

◆ CLR_bottom()

double NPSMEFTd6::CLR_bottom ( ) const

Definition at line 16529 of file NPSMEFTd6.cpp.

16530 {
16531  return (CLd_1133+CLd_3311);
16532 }

◆ CLR_charm()

double NPSMEFTd6::CLR_charm ( ) const

Definition at line 16519 of file NPSMEFTd6.cpp.

16520 {
16521  return (CLu_1122+CLu_2211);
16522 }

◆ CLR_down()

double NPSMEFTd6::CLR_down ( ) const

Definition at line 16514 of file NPSMEFTd6.cpp.

16515 {
16516  return (CLd_1111);
16517 }

◆ CLR_mu()

double NPSMEFTd6::CLR_mu ( ) const

Definition at line 16499 of file NPSMEFTd6.cpp.

16500 {
16501  return (CLe_1122+CLe_2211);
16502 }

◆ CLR_strange()

double NPSMEFTd6::CLR_strange ( ) const

Definition at line 16524 of file NPSMEFTd6.cpp.

16525 {
16526  return (CLd_1122+CLd_2211);
16527 }

◆ CLR_tau()

double NPSMEFTd6::CLR_tau ( ) const

Definition at line 16504 of file NPSMEFTd6.cpp.

16505 {
16506  return (CLe_1133+CLe_3311);
16507 }

◆ CLR_up()

double NPSMEFTd6::CLR_up ( ) const

Definition at line 16509 of file NPSMEFTd6.cpp.

16510 {
16511  return (CLu_1111);
16512 }

◆ computeGammaTotalRatio()

double NPSMEFTd6::computeGammaTotalRatio ( ) const
virtual

The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Reimplemented from NPbase.

Definition at line 10892 of file NPSMEFTd6.cpp.

10893 {
10894  double width = 1.0;
10895 
10896  width += dGammaHTotR1;
10897 
10898  if (FlagQuadraticTerms) {
10899  //Add contributions that are quadratic in the effective coefficients
10900  width += dGammaHTotR2;
10901  }
10902 
10903  if (width < 0) return std::numeric_limits<double>::quiet_NaN();
10904 
10905  return width;
10906 
10907 }

◆ CRL_bottom()

double NPSMEFTd6::CRL_bottom ( ) const

Definition at line 16564 of file NPSMEFTd6.cpp.

16565 {
16566  return (CQe_1133+CQe_3311);
16567 }

◆ CRL_charm()

double NPSMEFTd6::CRL_charm ( ) const

Definition at line 16554 of file NPSMEFTd6.cpp.

16555 {
16556  return (CQe_1122+CQe_2211);
16557 }

◆ CRL_down()

double NPSMEFTd6::CRL_down ( ) const

Definition at line 16549 of file NPSMEFTd6.cpp.

16550 {
16551  return (CQe_1111);
16552 }

◆ CRL_mu()

double NPSMEFTd6::CRL_mu ( ) const

Definition at line 16534 of file NPSMEFTd6.cpp.

16535 {
16536  return (CLe_1122+CLe_2211);
16537 }

◆ CRL_strange()

double NPSMEFTd6::CRL_strange ( ) const

Definition at line 16559 of file NPSMEFTd6.cpp.

16560 {
16561  return (CQe_1122+CQe_2211);
16562 }

◆ CRL_tau()

double NPSMEFTd6::CRL_tau ( ) const

Definition at line 16539 of file NPSMEFTd6.cpp.

16540 {
16541  return (CLe_1133+CLe_3311);
16542 }

◆ CRL_up()

double NPSMEFTd6::CRL_up ( ) const

Definition at line 16544 of file NPSMEFTd6.cpp.

16545 {
16546  return (CQe_1111);
16547 }

◆ CRR_bottom()

double NPSMEFTd6::CRR_bottom ( ) const

Definition at line 16600 of file NPSMEFTd6.cpp.

16601 {
16602  return (Ced_1133+Ced_3311);
16603 }

◆ CRR_charm()

double NPSMEFTd6::CRR_charm ( ) const

Definition at line 16590 of file NPSMEFTd6.cpp.

16591 {
16592  return (Ceu_1122+Ceu_2211);
16593 }

◆ CRR_down()

double NPSMEFTd6::CRR_down ( ) const

Definition at line 16585 of file NPSMEFTd6.cpp.

16586 {
16587  return (Ced_1111);
16588 }

◆ CRR_mu()

double NPSMEFTd6::CRR_mu ( ) const

Definition at line 16569 of file NPSMEFTd6.cpp.

16570 {
16571  return (Cee_1122+Cee_2211);
16572 }

◆ CRR_strange()

double NPSMEFTd6::CRR_strange ( ) const

Definition at line 16595 of file NPSMEFTd6.cpp.

16596 {
16597  return (Ced_1122+Ced_2211);
16598 }

◆ CRR_tau()

double NPSMEFTd6::CRR_tau ( ) const

Definition at line 16574 of file NPSMEFTd6.cpp.

16575 {
16576  return (Cee_1133+Cee_3311);
16577 }

◆ CRR_up()

double NPSMEFTd6::CRR_up ( ) const

Definition at line 16580 of file NPSMEFTd6.cpp.

16581 {
16582  return (Ceu_1111);
16583 }

◆ cZBox_HB()

double NPSMEFTd6::cZBox_HB ( ) const
virtual

The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{z\Box}\)

Reimplemented from NPbase.

Definition at line 15534 of file NPSMEFTd6.cpp.

15535 {
15536  double ciHB;
15537 
15538  ciHB = (sW2_tree/eeMz2)*( DeltaGF() + 0.5*CiHD*v2_over_LambdaNP2 );
15539 
15540  ciHB = ciHB + 0.5*(sW2_tree/eeMz)*(CiDHB / cW_tree + CiDHW / sW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
15541 
15542  return ciHB;
15543 }

◆ cZga_HB()

double NPSMEFTd6::cZga_HB ( ) const
virtual

The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{z\gamma}\)

Reimplemented from NPbase.

Definition at line 15558 of file NPSMEFTd6.cpp.

15559 {
15560  double ciHB;
15561 
15563 
15564  ciHB = ciHB + 0.5*(sW_tree*cW_tree/eeMz)*(CiDHB / sW_tree - CiDHW / cW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
15565 
15566  return ciHB;
15567 }

◆ cZZ_HB()

double NPSMEFTd6::cZZ_HB ( ) const
virtual

The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(c_{zz}\)

Reimplemented from NPbase.

Definition at line 15546 of file NPSMEFTd6.cpp.

15547 {
15548  double ciHB;
15549 
15551 
15552  ciHB = ciHB - (sW2_tree*cW2_tree/eeMz)*(CiDHB / cW_tree + CiDHW / sW_tree)*v2_over_LambdaNP2; // Extra, not in Warsaw basis
15553 
15554  return ciHB;
15555 }

◆ deltaa0()

double NPSMEFTd6::deltaa0 ( ) const
virtual

The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha(0)/\alpha(0)\)

Definition at line 3042 of file NPSMEFTd6.cpp.

3043 {
3044  // Ref. value fixed in SM EW fit 2018: from PDG 2018
3045  return ( (aleMz - 0.0072973525664) / 0.0072973525664 );
3046 }

◆ deltaa02()

double NPSMEFTd6::deltaa02 ( ) const
virtual

The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha(0)/\alpha(0))^2\)

Definition at line 3048 of file NPSMEFTd6.cpp.

3049 {
3050  return ( 0.0 );
3051 }

◆ deltaaMZ()

double NPSMEFTd6::deltaaMZ ( ) const
virtual

The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\)

Definition at line 3031 of file NPSMEFTd6.cpp.

3032 {
3033  // Ref. value from SM EW fit 2018
3034  return ( (aleMz - 0.007754941997887603) / 0.007754941997887603 );
3035 }

◆ deltaaMZ2()

double NPSMEFTd6::deltaaMZ2 ( ) const
virtual

The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\)

Definition at line 3037 of file NPSMEFTd6.cpp.

3038 {
3039  return ( 0.0 );
3040 }

◆ deltaaSMZ()

double NPSMEFTd6::deltaaSMZ ( ) const
virtual

The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\)

Definition at line 3053 of file NPSMEFTd6.cpp.

3054 {
3055  // Ref. value from SM EW fit 2018
3056  return ( (AlsMz - 0.1180) / 0.1180 );
3057 }

◆ deltaaSMZ2()

double NPSMEFTd6::deltaaSMZ2 ( ) const
virtual

The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\)

Definition at line 3059 of file NPSMEFTd6.cpp.

3060 {
3061  return ( 0.0 );
3062 }

◆ deltacZ_HB()

double NPSMEFTd6::deltacZ_HB ( ) const
virtual

The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta c_z\)

Reimplemented from NPbase.

Definition at line 15524 of file NPSMEFTd6.cpp.

15525 {
15526  double ciHB;
15527 
15528  ciHB = delta_h - (3.0/2.0)*DeltaGF();
15529 
15530  return ciHB;
15531 }

◆ deltaG1_hWW()

double NPSMEFTd6::deltaG1_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).

Returns
\(\delta g_{HWW}^{(1)}\)

Reimplemented from NPbase.

Definition at line 3258 of file NPSMEFTd6.cpp.

3259 {
3260  return (( 2.0 * CiHW - sqrt( M_PI * aleMz ) * CiDHW / sW_tree ) * v2_over_LambdaNP2 / v());
3261 }

◆ deltaG1_hZA()

double NPSMEFTd6::deltaG1_hZA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).

Returns
\(\delta g_{HZA}^{(1)}\)

Reimplemented from NPbase.

Definition at line 3296 of file NPSMEFTd6.cpp.

3297 {
3298  return ( (delta_AZ + 0.5 * sqrt( M_PI * aleMz ) * (CiDHB / sW_tree - CiDHW / cW_tree) * v2_over_LambdaNP2 )/ v());
3299 }

◆ deltaG1_hZARatio()

double NPSMEFTd6::deltaG1_hZARatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HZA}^{(1)}/g_{HZA}^{(1),SM}\)

Reimplemented from NPbase.

Definition at line 3301 of file NPSMEFTd6.cpp.

3302 {
3303  double m_t = mtpole;
3304  double m_b = quarks[BOTTOM].getMass();
3305  double m_c = quarks[CHARM].getMass();
3306  double m_tau = leptons[TAU].getMass();
3307  double m_mu = leptons[MU].getMass();
3308 
3309  double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
3310 
3311  double Qt = quarks[TOP].getCharge();
3312  double Qb = quarks[BOTTOM].getCharge();
3313  double Qc = quarks[CHARM].getCharge();
3314  double Qtau = leptons[TAU].getCharge();
3315  double Qmu = leptons[MU].getCharge();
3316 
3317  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
3318  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
3319  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
3320  double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
3321  double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
3322  double tau_W = 4.0 * M_w_2 / mHl / mHl;
3323 
3324  double lambda_t = 4.0 * m_t * m_t / Mz / Mz;
3325  double lambda_b = 4.0 * m_b * m_b / Mz / Mz;
3326  double lambda_c = 4.0 * m_c * m_c / Mz / Mz;
3327  double lambda_tau = 4.0 * m_tau * m_tau / Mz / Mz;
3328  double lambda_mu = 4.0 * m_mu * m_mu / Mz / Mz;
3329  double lambda_W = 4.0 * M_w_2 / Mz / Mz;
3330  double alpha2 = sqrt(2.0)*GF*M_w_2 / M_PI;
3331  double aPiv = sqrt(ale*alpha2) / 4.0 / M_PI / v();
3332 
3333 // mod. of Higgs couplings
3334  gslpp::complex gSM, dg;
3335  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3336  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3337  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3338  gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
3339  gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
3340  double dKappa_W = cLHd6 * (0.5 * v() / M_w_2)*deltaG3_hWW();
3341 
3342 // mod of EW vector couplings vf =2 gvf
3343  double vSMt = 2.0*(quarks[TOP].getIsospin()) - 4.0 * Qt * sW2_tree;
3344  double vSMb = 2.0*(quarks[BOTTOM].getIsospin()) - 4.0 * Qb * sW2_tree;
3345  double vSMc = 2.0*(quarks[CHARM].getIsospin()) - 4.0 * Qc * sW2_tree;
3346  double vSMtau = 2.0*(leptons[TAU].getIsospin()) - 4.0 * Qtau * sW2_tree;
3347  double vSMmu = 2.0*(leptons[MU].getIsospin()) - 4.0 * Qmu * sW2_tree;
3348 
3349  double dvSMt = cLHd6 * 2.0*deltaGV_f(quarks[TOP]);
3350  double dvSMb = cLHd6 * 2.0*deltaGV_f(quarks[BOTTOM]);
3351  double dvSMc = cLHd6 * 2.0*deltaGV_f(quarks[CHARM]);
3352  double dvSMtau = cLHd6 * 2.0*deltaGV_f(leptons[TAU]);
3353  double dvSMmu = cLHd6 * 2.0*deltaGV_f(leptons[MU]);
3354 
3355  double deltaloc = deltaG1_hZA();
3356 
3357  gSM = -aPiv * ((3.0*vSMt*Qt*AHZga_f(tau_t,lambda_t) +
3358  3.0*vSMb*Qb*AHZga_f(tau_b,lambda_b) +
3359  3.0*vSMc*Qc*AHZga_f(tau_c,lambda_c) +
3360  vSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
3361  vSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree +
3362  AHZga_W(tau_W,lambda_W));
3363 
3364  dg = deltaloc/gSM - (aPiv/gSM) * (
3365  (3.0*vSMt*dKappa_t*Qt*AHZga_f(tau_t,lambda_t) +
3366  3.0*vSMb*dKappa_b*Qb*AHZga_f(tau_b,lambda_b) +
3367  3.0*vSMc*dKappa_c*Qc*AHZga_f(tau_c,lambda_c)+
3368  dKappa_tau*vSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
3369  dKappa_mu*vSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree +
3370  dKappa_W*AHZga_W(tau_W,lambda_W) +
3371  (3.0*dvSMt*Qt*AHZga_f(tau_t,lambda_t) +
3372  3.0*dvSMb*Qb*AHZga_f(tau_b,lambda_b) +
3373  3.0*dvSMc*Qc*AHZga_f(tau_c,lambda_c)+
3374  dvSMtau*Qtau*AHZga_f(tau_tau,lambda_tau)+
3375  dvSMmu*Qmu*AHZga_f(tau_mu,lambda_mu))/cW_tree
3376  );
3377 
3378  return dg.real();
3379 }

◆ deltaG1_hZZ()

double NPSMEFTd6::deltaG1_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).

Returns
\(\delta g_{HZZ}^{(1)}\)

Reimplemented from NPbase.

Definition at line 3279 of file NPSMEFTd6.cpp.

3280 {
3281  return ( (delta_ZZ - 0.5 * sqrt( M_PI * aleMz ) * (CiDHB / cW_tree + CiDHW / sW_tree) * v2_over_LambdaNP2 )/ v());
3282 }

◆ deltag1ZNP()

double NPSMEFTd6::deltag1ZNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).

Returns
\(\delta g_{1,Z}\)

Reimplemented from NPbase.

Definition at line 13819 of file NPSMEFTd6.cpp.

13820 {
13821  double NPdirect, NPindirect;
13822 
13823  /* From own calculations. Agrees with with LHCHXWG-INT-2015-001 for common interactions */
13824  NPdirect = sW_tree / sqrt( 4.0 * M_PI * aleMz );
13825  NPdirect = - NPdirect * (Mz * Mz / v () / v() ) * CiDHW * v2_over_LambdaNP2;
13826 
13827  NPindirect = - 1.0 / (cW2_tree-sW2_tree);
13828 
13829  NPindirect = NPindirect * (sW_tree * CiHWB / cW_tree
13830  + 0.25 * CiHD ) * v2_over_LambdaNP2
13831  + 0.5 * NPindirect * DeltaGF() ;
13832 
13833  return NPdirect + NPindirect + dg1Z ;
13834 }

◆ deltag1ZNPEff()

double NPSMEFTd6::deltag1ZNPEff ( ) const
virtual

The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph].

Returns
\(\delta g_{1,Z}\)

Reimplemented from NPbase.

Definition at line 13862 of file NPSMEFTd6.cpp.

13863 {
13864  /* From arXiv:1708.09079 [hep-ph]. In our case, delta_e=0 since it is taken as inputs and its effects propagated
13865  * everywhere else */
13866  double dgEff;
13867 
13868  dgEff = (1.0/ cW2_tree) * ( (cW2_tree - sW2_tree)*deltaGL_f(leptons[ELECTRON])/gZlL +
13871 
13872  return dgEff + deltag1ZNP() ;
13873 }

◆ deltaG2_hWW()

double NPSMEFTd6::deltaG2_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).

Returns
\(\delta g_{HWW}^{(2)}\)

Reimplemented from NPbase.

Definition at line 3263 of file NPSMEFTd6.cpp.

3264 {
3265  return ( - sqrt( M_PI * aleMz ) * ( CiDHW / sW_tree ) * v2_over_LambdaNP2 / v());
3266 }

◆ deltaG2_hZA()

double NPSMEFTd6::deltaG2_hZA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).

Returns
\(\delta g_{HZA}^{(2)}\)

Reimplemented from NPbase.

Definition at line 3381 of file NPSMEFTd6.cpp.

3382 {
3383  return ( sqrt( M_PI * aleMz ) * ( CiDHB / sW_tree - CiDHW / cW_tree ) * v2_over_LambdaNP2 / v());
3384 }

◆ deltaG2_hZZ()

double NPSMEFTd6::deltaG2_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).

Returns
\(\delta g_{HZZ}^{(2)}\)

Reimplemented from NPbase.

Definition at line 3284 of file NPSMEFTd6.cpp.

3285 {
3286  return ( - sqrt( M_PI * aleMz ) * ( CiDHB / cW_tree + CiDHW / sW_tree ) * v2_over_LambdaNP2 / v());
3287 }

◆ deltaG3_hWW()

double NPSMEFTd6::deltaG3_hWW ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).

Returns
\(\delta g_{HWW}^{(3)}\)

Reimplemented from NPbase.

Definition at line 3268 of file NPSMEFTd6.cpp.

3269 {
3270  double NPindirect;
3271 
3272  NPindirect = 2.0 * cW2_tree * Mz * Mz / v()
3273  * (delta_h - 1.0 / 2.0 / (cW2_tree - sW2_tree)
3274  * ((4.0 * sW_tree * cW_tree * CiHWB + cW2_tree * CiHD) * v2_over_LambdaNP2 + DeltaGF()));
3275 
3276  return NPindirect;
3277 }

◆ deltaG3_hZZ()

double NPSMEFTd6::deltaG3_hZZ ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).

Returns
\(\delta g_{HZZ}^{(3)}\)

Reimplemented from NPbase.

Definition at line 3289 of file NPSMEFTd6.cpp.

3290 {
3291  double NPindirect = Mz * Mz / v() * (-0.5 * CiHD * v2_over_LambdaNP2 + delta_h - 0.5 * DeltaGF());
3292  double NPdirect = Mz * Mz / v() * CiHD * v2_over_LambdaNP2;
3293  return (NPindirect + NPdirect);
3294 }

◆ deltag3G()

double NPSMEFTd6::deltag3G ( ) const

The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).

Returns
\(\delta g_{3G}\)

Definition at line 3541 of file NPSMEFTd6.cpp.

3542 {
3543  /* Set to 0. for the moment */
3544 
3545  return 0.;
3546 }

◆ deltaG_Aff()

gslpp::complex NPSMEFTd6::deltaG_Aff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Aff}\)

Definition at line 3534 of file NPSMEFTd6.cpp.

3535 {
3536  /* Set to 0. for the moment */
3537 
3538  return 0.;
3539 }

◆ deltaG_Gff()

gslpp::complex NPSMEFTd6::deltaG_Gff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Gff}\)

Definition at line 3520 of file NPSMEFTd6.cpp.

3521 {
3522  /* Set to 0. for the moment */
3523 
3524  return 0.;
3525 }

◆ deltaG_hAA()

double NPSMEFTd6::deltaG_hAA ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).

Returns
\(\delta g_{HAA}\)

Reimplemented from NPbase.

Definition at line 3386 of file NPSMEFTd6.cpp.

3387 {
3388  return (delta_AA / v());
3389 }

◆ deltaG_hAARatio()

double NPSMEFTd6::deltaG_hAARatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HAA}/g_{HAA}^SM}\)

Reimplemented from NPbase.

Definition at line 3391 of file NPSMEFTd6.cpp.

3392 {
3393  double m_t = mtpole;
3394  double m_b = quarks[BOTTOM].getMass();
3395  double m_c = quarks[CHARM].getMass();
3396  double m_tau = leptons[TAU].getMass();
3397  double m_mu = leptons[MU].getMass();
3398 
3399  double M_w_2 = (trueSM.Mw())*(trueSM.Mw());
3400 
3401  double Qt = quarks[TOP].getCharge();
3402  double Qb = quarks[BOTTOM].getCharge();
3403  double Qc = quarks[CHARM].getCharge();
3404  double Qtau = leptons[TAU].getCharge();
3405  double Qmu = leptons[MU].getCharge();
3406 
3407  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
3408  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
3409  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
3410  double tau_tau = 4.0 * m_tau * m_tau / mHl / mHl;
3411  double tau_mu = 4.0 * m_mu * m_mu / mHl / mHl;
3412  double tau_W = 4.0 * M_w_2 / mHl / mHl;
3413 
3414  double aPiv = ale / 8.0 / M_PI / v();
3415  gslpp::complex gSM, dg;
3416  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3417  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3418  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3419  gslpp::complex dKappa_tau = cLHd6 * deltaG_hff(leptons[TAU]) / (-m_tau / v());
3420  gslpp::complex dKappa_mu = cLHd6 * deltaG_hff(leptons[MU]) / (-m_mu / v());
3421  double dKappa_W = cLHd6 * (0.5 * v() / M_w_2)*deltaG3_hWW();
3422 
3423  double deltaloc = deltaG_hAA();
3424 
3425  gSM = aPiv * (3.0*Qt*Qt*AH_f(tau_t) +
3426  3.0*Qb*Qb*AH_f(tau_b) +
3427  3.0*Qc*Qc*AH_f(tau_c) +
3428  Qtau*Qtau*AH_f(tau_tau) +
3429  Qmu*Qmu*AH_f(tau_mu) +
3430  AH_W(tau_W));
3431 
3432  dg = deltaloc/gSM + (aPiv/gSM) * (
3433  3.0*Qt*Qt*dKappa_t*AH_f(tau_t) +
3434  3.0*Qb*Qb*dKappa_b*AH_f(tau_b) +
3435  3.0*Qc*Qc*dKappa_c*AH_f(tau_c) +
3436  dKappa_tau*Qtau*Qtau*AH_f(tau_tau) +
3437  dKappa_mu*Qmu*Qmu*AH_f(tau_mu) +
3438  dKappa_W*AH_W(tau_W)
3439  );
3440 
3441  return dg.real();
3442 }

◆ deltaG_hAff()

gslpp::complex NPSMEFTd6::deltaG_hAff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hAff}\)

Definition at line 3513 of file NPSMEFTd6.cpp.

3514 {
3515  /* Set to 0. for the moment */
3516 
3517  return 0.;
3518 }

◆ deltaG_hff()

gslpp::complex NPSMEFTd6::deltaG_hff ( const Particle  p) const
virtual

The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Hff}\)

Reimplemented from NPbase.

Definition at line 3444 of file NPSMEFTd6.cpp.

3445 {
3446  /* The effects of the RG running are neglected. */
3447  double mf;
3448  if (p.is("TOP"))
3449  //mf = p.getMass(); // m_t(m_t)
3450  mf = mtpole; // pole mass
3451  else
3452  mf = p.getMass();
3453  gslpp::complex CfH = CfH_diag(p);
3454  return (-mf / v() * (delta_h - 0.5 * DeltaGF())
3455  + CfH * v2_over_LambdaNP2 / sqrt(2.0));
3456 }

◆ deltaG_hGff()

gslpp::complex NPSMEFTd6::deltaG_hGff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hGff}\)

Definition at line 3499 of file NPSMEFTd6.cpp.

3500 {
3501  /* Set to 0. for the moment */
3502 
3503  return 0.;
3504 }

◆ deltaG_hgg()

double NPSMEFTd6::deltaG_hgg ( ) const
virtual

The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).

Returns
\(\delta g_{HGG}\)

Reimplemented from NPbase.

Definition at line 3231 of file NPSMEFTd6.cpp.

3232 {
3233  return (CHG * v2_over_LambdaNP2 / v());
3234 }

◆ deltaG_hggRatio()

double NPSMEFTd6::deltaG_hggRatio ( ) const
virtual

The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.

Returns
\(\delta g_{HGG}/g_{HGG}^SM}\)

Reimplemented from NPbase.

Definition at line 3236 of file NPSMEFTd6.cpp.

3237 {
3238  double m_t = mtpole;
3239  double m_b = quarks[BOTTOM].getMass();
3240  double m_c = quarks[CHARM].getMass();
3241  double tau_t = 4.0 * m_t * m_t / mHl / mHl;
3242  double tau_b = 4.0 * m_b * m_b / mHl / mHl;
3243  double tau_c = 4.0 * m_c * m_c / mHl / mHl;
3244  double aSPiv = AlsMz / 16.0 / M_PI / v();
3245  gslpp::complex gSM, dg;
3246  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3247  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3248  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3249  double deltaloc = deltaG_hgg();
3250 
3251  gSM = aSPiv * (AH_f(tau_t) + AH_f(tau_b) + AH_f(tau_c));
3252 
3253  dg = deltaloc/gSM + (aSPiv/gSM) * (dKappa_t*AH_f(tau_t) + dKappa_b*AH_f(tau_b) + dKappa_c*AH_f(tau_c));
3254 
3255  return dg.real();
3256 }

◆ deltaG_hhhRatio()

double NPSMEFTd6::deltaG_hhhRatio ( ) const
virtual

The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.

Returns
\(\delta g_{HHH}/g_{HHH}^SM}\)

Reimplemented from NPbase.

Definition at line 3458 of file NPSMEFTd6.cpp.

3459 {
3460  double dg;
3461 
3462  dg = -0.5 * DeltaGF() + 3.0 * delta_h - 2.0 * CiH * v2_over_LambdaNP2 * v2/mHl/mHl;
3463 
3464  return dg;
3465 }

◆ deltaG_hZff()

gslpp::complex NPSMEFTd6::deltaG_hZff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{hZff}\)

Definition at line 3506 of file NPSMEFTd6.cpp.

3507 {
3508  /* Set to 0. for the moment */
3509 
3510  return 0.;
3511 }

◆ deltaG_Zff()

gslpp::complex NPSMEFTd6::deltaG_Zff ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{Zff}\)

Definition at line 3527 of file NPSMEFTd6.cpp.

3528 {
3529  /* Set to 0. for the moment */
3530 
3531  return 0.;
3532 }

◆ deltaGA_f()

double NPSMEFTd6::deltaGA_f ( const Particle  p) const
virtual

New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_A^f\)

Reimplemented from NPbase.

Definition at line 3171 of file NPSMEFTd6.cpp.

3172 {
3173  return (deltaGL_f(p) - deltaGR_f(p));
3174 }

◆ deltaGamma_W()

double NPSMEFTd6::deltaGamma_W ( ) const
virtual

The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).

Returns
\(\delta \Gamma_W\) in GeV

Reimplemented from NPbase.

Definition at line 3124 of file NPSMEFTd6.cpp.

3125 {
3126  double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
3127  double GammaW_tree = (3.0 + 2.0 * Nc) * G0;
3128 
3129  return (- 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
3130  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
3132  + 2.0 * (1.0 + cW2_tree) / 3.0 * DeltaGF())
3133  + 2.0 * G0 * (CiHL3_11 + CiHL3_22 + CiHL3_33 + Nc*(CiHQ3_11 + CiHQ3_22)) * v2_over_LambdaNP2);
3134 // + 2.0 * GammaW_tree / 3.0 * (CiHL3_11 + CiHQ3_11 + CiHQ3_22) * v2_over_LambdaNP2);
3135 }

◆ deltaGamma_Wff()

double NPSMEFTd6::deltaGamma_Wff ( const Particle  fi,
const Particle  fj 
) const
virtual

The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).

Parameters
[in]fia lepton or quark
[in]fja lepton or quark
Returns
\(\delta \Gamma_W^{ff}\) in GeV

Reimplemented from NPbase.

Definition at line 3090 of file NPSMEFTd6.cpp.

3091 {
3092  double G0 = GF * pow(Mz*cW_tree, 3.0) / 6.0 / sqrt(2.0) / M_PI;
3093  double deltaGamma_Wij;
3094  double GammaW_tree;
3095  double CHF3ij;
3096 
3097  if (fj.getIndex() - fi.getIndex() == 1)
3098  CHF3ij = CHF3_diag(fi);
3099  else
3100  CHF3ij = 0.;
3101 
3102  if (fi.is("QUARK")) {
3103  GammaW_tree = Nc * G0;
3104  } else {
3105  GammaW_tree = G0;
3106  }
3107 
3108  deltaGamma_Wij = - 3.0 * GammaW_tree / 4.0 / (cW2_tree - sW2_tree)
3109  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
3111  + 2.0 * (1.0 + cW2_tree) / 3.0 * DeltaGF());
3112 
3113  deltaGamma_Wij = deltaGamma_Wij + 2.0 * GammaW_tree * CHF3ij * v2_over_LambdaNP2;
3114 
3115  return deltaGamma_Wij;
3116 }

◆ deltaGammaHbbRatio1()

double NPSMEFTd6::deltaGammaHbbRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 12663 of file NPSMEFTd6.cpp.

12664 {
12665  double dwidth = 0.0;
12666 
12667  double C1 = 0.0;
12668 
12669  if (FlagLoopHd6) {
12670 
12671  dwidth = ( +121248. * CiHbox / LambdaNP2
12672  -558.186 * CiuH_33r / LambdaNP2
12673  -5027051. * CidH_33r / LambdaNP2
12674  -30312.1 * CiHD / LambdaNP2
12675  -60624.1 * DeltaGF() / v() / v() );
12676 
12677  } else {
12678 
12679  dwidth = ( +121248. * CiHbox / LambdaNP2
12680  -5050180. * CidH_33r / LambdaNP2
12681  -30312.1 * CiHD / LambdaNP2
12682  -60624.1 * DeltaGF() / v() / v() );
12683  }
12684 
12685 // Linear contribution from Higgs self-coupling
12686  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12687 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12688  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12689 
12690  // Add modifications due to small variations of the SM parameters
12691  dwidth += cHSM * ( +1. * deltaGmu()
12692  -0.23 * deltaaSMZ()
12693  +1.007 * deltaMh()
12694  +0.001 * deltamt()
12695  +1.992 * deltamb() );
12696 
12697  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12698  dwidth += eHbbint + eHbbpar;
12699 
12700  return dwidth;
12701 }

◆ deltaGammaHbbRatio2()

double NPSMEFTd6::deltaGammaHbbRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 12703 of file NPSMEFTd6.cpp.

12704 {
12705  double dwidth = 0.0;
12706 
12707 
12708  //Contributions that are quadratic in the effective coefficients
12709  return ( dwidth );
12710 
12711 }

◆ deltaGammaHccRatio1()

double NPSMEFTd6::deltaGammaHccRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 12598 of file NPSMEFTd6.cpp.

12599 {
12600  double dwidth = 0.0;
12601 
12602  double C1 = 0.0;
12603 
12604  if (FlagLoopHd6) {
12605 
12606  dwidth = ( +121248. * CiHbox / LambdaNP2
12607  -16421890. * CiuH_22r / LambdaNP2
12608  -992.159 * CiuH_33r / LambdaNP2
12609  -30312.1 * CiHD / LambdaNP2
12610  -60624.1 * DeltaGF() / v() / v() );
12611 
12612  } else {
12613 
12614  dwidth = ( +121248. * CiHbox / LambdaNP2
12615  -16556668. * CiuH_22r / LambdaNP2
12616  -30312.1 * CiHD / LambdaNP2
12617  -60624.1 * DeltaGF() / v() / v() );
12618  }
12619 
12620 // Linear contribution from Higgs self-coupling
12621  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12622 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12623  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12624 
12625  // Add modifications due to small variations of the SM parameters
12626  dwidth += cHSM * ( +1. * deltaGmu()
12627  -0.789 * deltaaSMZ()
12628  +1.004 * deltaMh()
12629  +0.001 * deltamt()
12630  +1.995 * deltamc() );
12631 
12632  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12633  dwidth += eHccint + eHccpar;
12634 
12635  return dwidth;
12636 }

◆ deltaGammaHccRatio2()

double NPSMEFTd6::deltaGammaHccRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 12638 of file NPSMEFTd6.cpp.

12639 {
12640  double dwidth = 0.0;
12641 
12642 
12643  //Contributions that are quadratic in the effective coefficients
12644  return ( dwidth );
12645 
12646 }

◆ deltaGammaHgagaRatio1()

double NPSMEFTd6::deltaGammaHgagaRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 12417 of file NPSMEFTd6.cpp.

12418 {
12419  double dwidth = 0.0;
12420 
12421  double C1 = 0.0049;
12422 
12423 // It does not include modifications of MW
12424 
12425 // Write the tree-level contributions directly as a function
12426 // of delta_AA (or deltaG_hAA) to account for variations of sw2 and cw2
12427 
12428  dwidth = ( -255156.97*deltaG_hAA()
12429 // -48314158. * CiHB / LambdaNP2
12430 // -14510502. * CiHW / LambdaNP2
12431 // +26477588. * CiHWB / LambdaNP2
12432  + cLHd6 * (
12433  +119766. * CiHbox / LambdaNP2
12434  -42565.7 * CieH_33r / LambdaNP2
12435  -48868.1 * CiuH_22r / LambdaNP2
12436  +32078.2 * CiuH_33r / LambdaNP2
12437  -18428.3 * CidH_33r / LambdaNP2
12438  -137452. * CiHD / LambdaNP2
12439  -235677. * CiHWB / LambdaNP2
12440  -124462. * DeltaGF() / v() / v()
12441  -1.257 * deltaMwd6() )
12442  );
12443 
12444 // Linear contribution from Higgs self-coupling
12445  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12446 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12447  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12448 
12449  // Add modifications due to small variations of the SM parameters
12450  dwidth += cHSM * ( +2. * deltaa0()
12451  +0.27 * deltaaMZ()
12452  +0.736 * deltaGmu()
12453  -1.797 * deltaMz()
12454  +0.02 * deltaaSMZ()
12455  +4.195 * deltaMh()
12456  +0.047 * deltamt()
12457  +0.008 * deltamb()
12458  +0.009 * deltamc()
12459  +0.01 * deltamtau() );
12460 
12461  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12462  dwidth += eHgagaint + eHgagapar;
12463 
12464  return dwidth;
12465 }

◆ deltaGammaHgagaRatio2()

double NPSMEFTd6::deltaGammaHgagaRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 12467 of file NPSMEFTd6.cpp.

12468 {
12469  double dwidth = 0.0;
12470 
12471 
12472  //Contributions that are quadratic in the effective coefficients
12473  return ( dwidth );
12474 
12475 }

◆ deltaGammaHggRatio1()

double NPSMEFTd6::deltaGammaHggRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 10988 of file NPSMEFTd6.cpp.

10989 {
10990  double dwidth = 0.0;
10991 
10992  double C1 = 0.0066;
10993 
10994  dwidth = ( +37526258. * CHG / LambdaNP2
10995  + cLHd6 * (
10996  +121248. * CiHbox / LambdaNP2
10997  +173353. * CiuH_22r / LambdaNP2
10998  -129155. * CiuH_33r / LambdaNP2
10999  +248530. * CidH_33r / LambdaNP2
11000  -30312.1 * CiHD / LambdaNP2
11001  -60624.1 * DeltaGF() / v() / v() )
11002  );
11003 
11004 // Linear contribution from Higgs self-coupling
11005  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11006 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11007  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11008 
11009  // Add modifications due to small variations of the SM parameters
11010  dwidth += cHSM * ( +1.003 * deltaGmu()
11011  +2.31 * deltaaSMZ()
11012  +3.276 * deltaMh()
11013  -0.134 * deltamt()
11014  -0.106 * deltamb()
11015  -0.03 * deltamc() );
11016 
11017  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11018  dwidth += eHggint + eHggpar;
11019 
11020  return dwidth;
11021 }

◆ deltaGammaHggRatio2()

double NPSMEFTd6::deltaGammaHggRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 11023 of file NPSMEFTd6.cpp.

11024 {
11025  double dwidth = 0.0;
11026 
11027 
11028  //Contributions that are quadratic in the effective coefficients
11029  return ( dwidth );
11030 
11031 }

◆ deltaGammaHmumuRatio1()

double NPSMEFTd6::deltaGammaHmumuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 12493 of file NPSMEFTd6.cpp.

12494 {
12495  double dwidth = 0.0;
12496 
12497  double C1 = 0.0;
12498 
12499  dwidth = ( +121248. * CiHbox / LambdaNP2
12500  -199792511. * CieH_22r / LambdaNP2
12501  -30312.1 * CiHD / LambdaNP2
12502  -60624.1 * DeltaGF() / v() / v() );
12503 
12504 // Linear contribution from Higgs self-coupling
12505  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12506 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12507  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12508 
12509  // Add modifications due to small variations of the SM parameters
12510  dwidth += cHSM * ( +1. * deltaGmu()
12511  +1. * deltaMh() );
12512 
12513  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12514  dwidth += eHmumuint + eHmumupar;
12515 
12516  return dwidth;
12517 }

◆ deltaGammaHmumuRatio2()

double NPSMEFTd6::deltaGammaHmumuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 12519 of file NPSMEFTd6.cpp.

12520 {
12521  double dwidth = 0.0;
12522 
12523 
12524  //Contributions that are quadratic in the effective coefficients
12525  return ( dwidth );
12526 
12527 }

◆ deltaGammaHtautauRatio1()

double NPSMEFTd6::deltaGammaHtautauRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 12545 of file NPSMEFTd6.cpp.

12546 {
12547  double dwidth = 0.0;
12548 
12549  double C1 = 0.0;
12550 
12551  dwidth = ( +121248. * CiHbox / LambdaNP2
12552  -11880369. * CieH_33r / LambdaNP2
12553  -30312.1 * CiHD / LambdaNP2
12554  -60624.1 * DeltaGF() / v() / v() );
12555 
12556 // Linear contribution from Higgs self-coupling
12557  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12558 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12559  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12560 
12561  // Add modifications due to small variations of the SM parameters
12562  dwidth += cHSM * ( +1. * deltaGmu()
12563  +1.002 * deltaMh()
12564  +1.998 * deltamtau() );
12565 
12566  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12567  dwidth += eHtautauint + eHtautaupar;
12568 
12569  return dwidth;
12570 }

◆ deltaGammaHtautauRatio2()

double NPSMEFTd6::deltaGammaHtautauRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 12572 of file NPSMEFTd6.cpp.

12573 {
12574  double dwidth = 0.0;
12575 
12576 
12577  //Contributions that are quadratic in the effective coefficients
12578  return ( dwidth );
12579 
12580 }

◆ deltaGammaHWffRatio1()

double NPSMEFTd6::deltaGammaHWffRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 11330 of file NPSMEFTd6.cpp.

11331 {
11332  double dwidth = 0.0;
11333 
11334  double C1 = 0.0073;
11335 
11336  dwidth = ( +121288. * CiHbox / LambdaNP2
11337  +5395.21 * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
11338  +11680.9 * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
11339  -159787. * CiHD / LambdaNP2
11340  -91509.1 * CiHW / LambdaNP2
11341  -283092. * CiHWB / LambdaNP2
11342  +37845.1 * CiDHW / LambdaNP2
11343  -3.259 * DeltaGF()
11344  -15.196 * deltaMwd6() );
11345 
11346 // Linear contribution from Higgs self-coupling
11347  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11348 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11349  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11350 
11351  // Add modifications due to small variations of the SM parameters
11352  //dwidth += cHSM * ( 0.0 );
11353 
11354  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11355  //dwidth += eHWWint + eHWWpar;
11356 
11357  return dwidth;
11358 
11359 }

◆ deltaGammaHWffRatio2()

double NPSMEFTd6::deltaGammaHWffRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 11361 of file NPSMEFTd6.cpp.

11362 {
11363  double dwidth = 0.0;
11364 
11365 
11366  //Contributions that are quadratic in the effective coefficients
11367  return ( dwidth );
11368 
11369 }

◆ deltaGammaHWjjRatio1()

double NPSMEFTd6::deltaGammaHWjjRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 11214 of file NPSMEFTd6.cpp.

11215 {
11216  double dwidth = 0.0;
11217 
11218  double C1 = 0.0073;
11219 
11220  dwidth = ( +121611. * CiHbox / LambdaNP2
11221  +17701.4 * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
11222  -159273. * CiHD / LambdaNP2
11223  -91021.6 * CiHW / LambdaNP2
11224  -282574. * CiHWB / LambdaNP2
11225  +37917.5 * CiDHW / LambdaNP2
11226  -3.259 * DeltaGF()
11227  -15.198 * deltaMwd6() );
11228 
11229 // Linear contribution from Higgs self-coupling
11230  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11231 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11232  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11233 
11234  // Add modifications due to small variations of the SM parameters
11235  //dwidth += cHSM * ( 0.0 );
11236 
11237  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11238  //dwidth += eHWWint + eHWWpar;
11239 
11240  return dwidth;
11241 
11242 }

◆ deltaGammaHWjjRatio2()

double NPSMEFTd6::deltaGammaHWjjRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 11244 of file NPSMEFTd6.cpp.

11245 {
11246  double dwidth = 0.0;
11247 
11248 
11249  //Contributions that are quadratic in the effective coefficients
11250  return ( dwidth );
11251 
11252 }

◆ deltaGammaHWlvRatio1()

double NPSMEFTd6::deltaGammaHWlvRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 11097 of file NPSMEFTd6.cpp.

11098 {
11099  double dwidth = 0.0;
11100 
11101  double C1 = 0.0073;
11102 
11103  dwidth = ( +121875. * CiHbox / LambdaNP2
11104  +18351.9 * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
11105  -159873. * CiHD / LambdaNP2
11106  -91288.7 * CiHW / LambdaNP2
11107  -284689. * CiHWB / LambdaNP2
11108  +37703.7 * CiDHW / LambdaNP2
11109  -3.292 * DeltaGF()
11110  -15.14 * deltaMwd6() );
11111 
11112 // Linear contribution from Higgs self-coupling
11113  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11114 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11115  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11116 
11117  // Add modifications due to small variations of the SM parameters
11118  //dwidth += cHSM * ( 0.0 );
11119 
11120  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11121  //dwidth += eHWWint + eHWWpar;
11122 
11123  return dwidth;
11124 
11125 }

◆ deltaGammaHWlvRatio2()

double NPSMEFTd6::deltaGammaHWlvRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 11127 of file NPSMEFTd6.cpp.

11128 {
11129  double dwidth = 0.0;
11130 
11131 
11132  //Contributions that are quadratic in the effective coefficients
11133  return ( dwidth );
11134 
11135 }

◆ deltaGammaHWW2l2vRatio1()

double NPSMEFTd6::deltaGammaHWW2l2vRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 11153 of file NPSMEFTd6.cpp.

11154 {
11155  double dwidth = 0.0;
11156 
11157  double C1 = 0.0073;
11158 
11159  dwidth = ( +120742. * CiHbox / LambdaNP2
11160  +131582. * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
11161  -204043. * CiHD / LambdaNP2
11162  -91463.9 * CiHW / LambdaNP2
11163  -379529. * CiHWB / LambdaNP2
11164  +36848.2 * CiDHW / LambdaNP2
11165  -4.705 * DeltaGF()
11166  -13.735 * deltaMwd6()
11167  -0.965 * deltaGwd6()
11168  );
11169 
11170 // Linear contribution from Higgs self-coupling
11171  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11172 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11173  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11174 
11175  // Add modifications due to small variations of the SM parameters
11176  dwidth += cHSM * ( -12.123 * deltaMz()
11177  +13.615 * deltaMh()
11178  +1.756 * deltaaMZ()
11179  +0.216 * deltaGmu() );
11180 
11181  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11182  dwidth += eHWWint + eHWWpar;
11183 
11184  return dwidth;
11185 
11186 }

◆ deltaGammaHWW2l2vRatio2()

double NPSMEFTd6::deltaGammaHWW2l2vRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 11188 of file NPSMEFTd6.cpp.

11189 {
11190  double dwidth = 0.0;
11191 
11192 
11193  //Contributions that are quadratic in the effective coefficients
11194  return ( dwidth );
11195 
11196 }

◆ deltaGammaHWW4fRatio1()

double NPSMEFTd6::deltaGammaHWW4fRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 11387 of file NPSMEFTd6.cpp.

11388 {
11389  double dwidth = 0.0;
11390 
11391  double C1 = 0.0073;
11392 
11393  double CWff, sf;
11394 
11395  CWff = ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) * v2_over_LambdaNP2 +
11397 
11398  CWff = CWff/( 3.0 + 2.0*Nc );
11399 
11400  sf = 90362.5 * (1.0/2.0) * ( 3.0 + 2.0*Nc )/(Nc*v2) ; // Coefficient of the CWff term. From the CiHQ3_11 term in the ME.
11401 
11402  dwidth = ( +121886. * CiHbox / LambdaNP2
11403  + sf* CWff
11404  -204009. * CiHD / LambdaNP2
11405  -91455.7 * CiHW / LambdaNP2
11406  -382903. * CiHWB / LambdaNP2
11407  +38314.9 * CiDHW / LambdaNP2
11408  -4.757 * DeltaGF()
11409  -13.716 * deltaMwd6()
11410  -0.963 * deltaGwd6()
11411  );
11412 
11413 // Linear contribution from Higgs self-coupling
11414  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11415 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11416  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11417 
11418  // Add modifications due to small variations of the SM parameters
11419  dwidth += cHSM * ( -12.271 * deltaMz()
11420  +13.665 * deltaMh()
11421  +1.85 * deltaaMZ()
11422  +0.224 * deltaGmu() );
11423 
11424  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11425  dwidth += eHWWint + eHWWpar;
11426 
11427  return dwidth;
11428 
11429 }

◆ deltaGammaHWW4fRatio2()

double NPSMEFTd6::deltaGammaHWW4fRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 11431 of file NPSMEFTd6.cpp.

11432 {
11433  double dwidth = 0.0;
11434 
11435 
11436  //Contributions that are quadratic in the effective coefficients
11437  return ( dwidth );
11438 
11439 }

◆ deltaGammaHWW4jRatio1()

double NPSMEFTd6::deltaGammaHWW4jRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 11270 of file NPSMEFTd6.cpp.

11271 {
11272  double dwidth = 0.0;
11273 
11274  double C1 = 0.0073;
11275 
11276  dwidth = ( +121936. * CiHbox / LambdaNP2
11277  +138860. * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
11278  -205023. * CiHD / LambdaNP2
11279  -89938.5 * CiHW / LambdaNP2
11280  -383944. * CiHWB / LambdaNP2
11281  +38244.6 * CiDHW / LambdaNP2
11282  -4.816 * DeltaGF()
11283  -13.647 * deltaMwd6()
11284  -0.959 * deltaGwd6() );
11285 
11286 // Linear contribution from Higgs self-coupling
11287  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11288 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11289  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11290 
11291  // Add modifications due to small variations of the SM parameters
11292  dwidth += cHSM * ( -12.168 * deltaMz()
11293  +13.66 * deltaMh()
11294  +1.899 * deltaaMZ()
11295  +0.189 * deltaGmu() );
11296 
11297  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11298  dwidth += eHWWint + eHWWpar;
11299 
11300  return dwidth;
11301 
11302 }

◆ deltaGammaHWW4jRatio2()

double NPSMEFTd6::deltaGammaHWW4jRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 11304 of file NPSMEFTd6.cpp.

11305 {
11306  double dwidth = 0.0;
11307 
11308 
11309  //Contributions that are quadratic in the effective coefficients
11310  return ( dwidth );
11311 
11312 }

◆ deltaGammaHWWRatio1()

double NPSMEFTd6::deltaGammaHWWRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 11049 of file NPSMEFTd6.cpp.

11050 {
11051  double dwidth = 0.0;
11052 
11053 // double C1 = 0.0073;
11054 
11055  dwidth = deltaGammaHWW4fRatio1();
11056 
11057 // Linear contribution from Higgs self-coupling
11058 // dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11059 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11060 // dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11061 
11062  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11063 // dwidth += eHWWint + eHWWpar;
11064 
11065  return dwidth;
11066 
11067 }

◆ deltaGammaHWWRatio2()

double NPSMEFTd6::deltaGammaHWWRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 11069 of file NPSMEFTd6.cpp.

11070 {
11071  double dwidth = 0.0;
11072 
11073  //Contributions that are quadratic in the effective coefficients
11074  dwidth = deltaGammaHWW4fRatio2();
11075 
11076 
11077  return dwidth;
11078 
11079 }

◆ deltaGammaHZddRatio1()

double NPSMEFTd6::deltaGammaHZddRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z d d)\)/ \(\Gamma(H\to Z d d)_{\mathrm{SM}}\)

Definition at line 12124 of file NPSMEFTd6.cpp.

12125 {
12126  double dwidth = 0.0;
12127 
12128  double C1 = 0.0083;
12129 
12130  dwidth = ( +121756. * CiHbox / LambdaNP2
12131  +9252.73 * (1.0/3.0) * ( CiHQ1_11 + CiHQ1_22 + CiHQ1_33 ) / LambdaNP2
12132  -1471.03 * (1.0/3.0) * ( CiHd_11 + CiHd_22 + CiHd_33 ) / LambdaNP2
12133  +9252.73 * (1.0/3.0) * ( CiHQ3_11 + CiHQ3_22 + CiHQ3_33 ) / LambdaNP2
12134  -12714.3 * CiHD / LambdaNP2
12135  -13589.3 * CiHB / LambdaNP2
12136  -45689.4 * CiHW / LambdaNP2
12137  -85582.3 * CiHWB / LambdaNP2
12138  +17007.1 * CiDHB / LambdaNP2
12139  +30733.1 * CiDHW / LambdaNP2
12140  -2.427 * DeltaGF() );
12141 
12142 // Linear contribution from Higgs self-coupling
12143  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12144 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12145  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12146 
12147  // Add modifications due to small variations of the SM parameters
12148  //dwidth += cHSM * ( 0.0 );
12149 
12150  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12151  //dwidth += eHZZint + eHZZpar;
12152 
12153  return dwidth;
12154 
12155 }

◆ deltaGammaHZddRatio2()

double NPSMEFTd6::deltaGammaHZddRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z d d)\)/ \(\Gamma(H\to Z d d)_{\mathrm{SM}}\)

Definition at line 12157 of file NPSMEFTd6.cpp.

12158 {
12159  double dwidth = 0.0;
12160 
12161 
12162  //Contributions that are quadratic in the effective coefficients
12163  return ( dwidth );
12164 
12165 }

◆ deltaGammaHZeeRatio1()

double NPSMEFTd6::deltaGammaHZeeRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 11564 of file NPSMEFTd6.cpp.

11565 {
11566  double dwidth = 0.0;
11567 
11568  double C1 = 0.0083;
11569 
11570 // Derived from the HZll expression for l=e only
11571 
11572  dwidth = ( +121715. * CiHbox / LambdaNP2
11573  +8726.9 * CiHL1_11 / LambdaNP2
11574  -7315.2 * CiHe_11 / LambdaNP2
11575  +8726.9 * CiHL3_11 / LambdaNP2
11576  -5544.15 * CiHD / LambdaNP2
11577  -13560.9 * CiHB / LambdaNP2
11578  -45585.2 * CiHW / LambdaNP2
11579  -53507.9 * CiHWB / LambdaNP2
11580  +16829.2 * CiDHB / LambdaNP2
11581  +30766.6 * CiDHW / LambdaNP2
11582  -2.204 * DeltaGF() );
11583 
11584 // Linear contribution from Higgs self-coupling
11585  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11586 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11587  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11588 
11589  // Add modifications due to small variations of the SM parameters
11590  //dwidth += cHSM * ( 0.0 );
11591 
11592  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11593  //dwidth += eHZZint + eHZZpar;
11594 
11595  return dwidth;
11596 
11597 }

◆ deltaGammaHZeeRatio2()

double NPSMEFTd6::deltaGammaHZeeRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 11599 of file NPSMEFTd6.cpp.

11600 {
11601  double dwidth = 0.0;
11602 
11603 
11604  //Contributions that are quadratic in the effective coefficients
11605  return ( dwidth );
11606 
11607 }

◆ deltaGammaHZffRatio1()

double NPSMEFTd6::deltaGammaHZffRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z f f)\)/ \(\Gamma(H\to Z f f)_{\mathrm{SM}}\)

Definition at line 12183 of file NPSMEFTd6.cpp.

12184 {
12185  double dwidth = 0.0;
12186 
12187  double C1 = 0.0083;
12188 
12189  dwidth = ( +121551. * CiHbox / LambdaNP2
12190  -824.482 * (1.0/3.0) * ( CiHL1_11 + CiHL1_22 + CiHL1_33 ) / LambdaNP2
12191  +1840.54 * (1.0/12.0) * ( 5.0 * CiHQ1_11 + 5.0 * CiHQ1_22 + 2.0 * CiHQ1_33 - CiHQ3_11 - CiHQ3_22 + 2.0 * CiHQ3_33 ) / LambdaNP2
12192  -795.383 * (1.0/3.0) * ( CiHe_11 + CiHe_22 + CiHe_33 ) / LambdaNP2
12193  +1069.4 * (1.0/2.0) * ( CiHu_11 + CiHu_22 ) / LambdaNP2
12194  -579.563 * (1.0/3.0) * ( CiHd_11 + CiHd_22 + CiHd_33 ) / LambdaNP2
12195  +3164.56 * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
12196  +6413.99 * (-1.0/12.0) * ( CiHQ1_11 + CiHQ1_22 - 2.0 * CiHQ1_33 - 5.0 * CiHQ3_11 - 5.0 * CiHQ3_22 - 2.0 * CiHQ3_33) / LambdaNP2
12197  -10839.5 * CiHD / LambdaNP2
12198  -14222.3 * CiHB / LambdaNP2
12199  -45455.6 * CiHW / LambdaNP2
12200  -75343.1 * CiHWB / LambdaNP2
12201  +16804.9 * CiDHB / LambdaNP2
12202  +30421. * CiDHW / LambdaNP2
12203  -2.356 * DeltaGF() );
12204 
12205 // Linear contribution from Higgs self-coupling
12206  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12207 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12208  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12209 
12210  // Add modifications due to small variations of the SM parameters
12211  //dwidth += cHSM * ( 0.0 );
12212 
12213  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12214  //dwidth += eHZZint + eHZZpar;
12215 
12216  return dwidth;
12217 
12218 }

◆ deltaGammaHZffRatio2()

double NPSMEFTd6::deltaGammaHZffRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z f f)\)/ \(\Gamma(H\to Z f f)_{\mathrm{SM}}\)

Definition at line 12220 of file NPSMEFTd6.cpp.

12221 {
12222  double dwidth = 0.0;
12223 
12224 
12225  //Contributions that are quadratic in the effective coefficients
12226  return ( dwidth );
12227 
12228 }

◆ deltaGammaHZgaRatio1()

double NPSMEFTd6::deltaGammaHZgaRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 12332 of file NPSMEFTd6.cpp.

12333 {
12334  double dwidth = 0.0;
12335 
12336  double C1 = 0.0;
12337 
12338 // It includes modifications of Zff vertices and MW, but not on the pure VVV and VVVV vertices
12339 
12340 // Write the tree-level contributions directly as a function
12341 // of delta_ZA (or deltaG1_hZA()) to account for variations of sw2 and cw2
12342 
12343  dwidth = ( -71769.02 * deltaG1_hZA()
12344 // +14894914. * CiHB / LambdaNP2
12345 // -14894913. * CiHW / LambdaNP2
12346 // +9508089. * CiHWB / LambdaNP2
12347 // -2869576. * CiDHB / LambdaNP2
12348 // +1572613. * CiDHW / LambdaNP2
12349  + cLHd6 * (
12350  +120002. * CiHbox / LambdaNP2
12351  +50.12 * CiHL1_33 / LambdaNP2
12352  +17401. * CiHQ1_33 / LambdaNP2
12353  +50.12 * CiHe_33 / LambdaNP2
12354  +17188.7 * CiHu_33 / LambdaNP2
12355  +212.376 * CiHd_33 / LambdaNP2
12356  +50.12 * CiHL3_33 / LambdaNP2
12357  -16976.3 * CiHQ3_33 / LambdaNP2
12358  -373.856 * CieH_33r / LambdaNP2
12359  -2953.05 * CiuH_22r / LambdaNP2
12360  +6636.34 * CiuH_33r / LambdaNP2
12361  -6121.66 * CidH_33r / LambdaNP2
12362  -111254. * CiHD / LambdaNP2
12363  -162538. * CiHWB / LambdaNP2
12364  -96076.1 * DeltaGF() / v() / v()
12365  -0.123 * deltaMwd6() )
12366  );
12367 
12368 // Linear contribution from Higgs self-coupling
12369  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12370 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12371  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12372 
12373  // Add modifications due to small variations of the SM parameters
12374  dwidth += cHSM * ( +1. * deltaa0()
12375  -0.629 * deltaaMZ()
12376  +2.629 * deltaGmu()
12377  -4.926 * deltaMz()
12378  +0.004 * deltaaSMZ()
12379  +11.167 * deltaMh()
12380  +0.013 * deltamt()
12381  +0.004 * deltamb()
12382  +0.001 * deltamc()
12383  +0. * deltamtau() );
12384 
12385  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12386  dwidth += eHZgaint + eHZgapar;
12387 
12388  return dwidth;
12389 }

◆ deltaGammaHZgaRatio2()

double NPSMEFTd6::deltaGammaHZgaRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 12391 of file NPSMEFTd6.cpp.

12392 {
12393  double dwidth = 0.0;
12394 
12395 
12396  //Contributions that are quadratic in the effective coefficients
12397  return ( dwidth );
12398 
12399 }

◆ deltaGammaHZllRatio1()

double NPSMEFTd6::deltaGammaHZllRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 11505 of file NPSMEFTd6.cpp.

11506 {
11507  double dwidth = 0.0;
11508 
11509  double C1 = 0.0083;
11510 
11511  dwidth = ( +121715. * CiHbox / LambdaNP2
11512  +8726.9 * (1.0/2.0) * ( CiHL1_11 + CiHL1_22 ) / LambdaNP2
11513  -7315.2 * (1.0/2.0) * ( CiHe_11 + CiHe_22 ) / LambdaNP2
11514  +8726.9 * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
11515  -5544.15 * CiHD / LambdaNP2
11516  -13560.9 * CiHB / LambdaNP2
11517  -45585.2 * CiHW / LambdaNP2
11518  -53507.9 * CiHWB / LambdaNP2
11519  +16829.2 * CiDHB / LambdaNP2
11520  +30766.6 * CiDHW / LambdaNP2
11521  -2.204 * DeltaGF() );
11522 
11523 // Linear contribution from Higgs self-coupling
11524  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11525 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11526  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11527 
11528  // Add modifications due to small variations of the SM parameters
11529  //dwidth += cHSM * ( 0.0 );
11530 
11531  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11532  //dwidth += eHZZint + eHZZpar;
11533 
11534  return dwidth;
11535 
11536 }

◆ deltaGammaHZllRatio2()

double NPSMEFTd6::deltaGammaHZllRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 11538 of file NPSMEFTd6.cpp.

11539 {
11540  double dwidth = 0.0;
11541 
11542 
11543  //Contributions that are quadratic in the effective coefficients
11544  return ( dwidth );
11545 
11546 }

◆ deltaGammaHZmumuRatio1()

double NPSMEFTd6::deltaGammaHZmumuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 11625 of file NPSMEFTd6.cpp.

11626 {
11627  double dwidth = 0.0;
11628 
11629  double C1 = 0.0083;
11630 
11631 // Derived from the HZll expression for l=mu only
11632 
11633  dwidth = ( +121715. * CiHbox / LambdaNP2
11634  +8726.9 * CiHL1_22 / LambdaNP2
11635  -7315.2 * CiHe_22 / LambdaNP2
11636  +8726.9 * CiHL3_22 / LambdaNP2
11637  -5544.15 * CiHD / LambdaNP2
11638  -13560.9 * CiHB / LambdaNP2
11639  -45585.2 * CiHW / LambdaNP2
11640  -53507.9 * CiHWB / LambdaNP2
11641  +16829.2 * CiDHB / LambdaNP2
11642  +30766.6 * CiDHW / LambdaNP2
11643  -2.204 * DeltaGF() );
11644 
11645 // Linear contribution from Higgs self-coupling
11646  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11647 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11648  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11649 
11650  // Add modifications due to small variations of the SM parameters
11651  //dwidth += cHSM * ( 0.0 );
11652 
11653  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11654  //dwidth += eHZZint + eHZZpar;
11655 
11656  return dwidth;
11657 
11658 }

◆ deltaGammaHZmumuRatio2()

double NPSMEFTd6::deltaGammaHZmumuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 11660 of file NPSMEFTd6.cpp.

11661 {
11662  double dwidth = 0.0;
11663 
11664 
11665  //Contributions that are quadratic in the effective coefficients
11666  return ( dwidth );
11667 
11668 }

◆ deltaGammaHZuuRatio1()

double NPSMEFTd6::deltaGammaHZuuRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z u u)\)/ \(\Gamma(H\to Z u u)_{\mathrm{SM}}\)

Definition at line 12065 of file NPSMEFTd6.cpp.

12066 {
12067  double dwidth = 0.0;
12068 
12069  double C1 = 0.0083;
12070 
12071  dwidth = ( +121512. * CiHbox / LambdaNP2
12072  -9648.28 * (1.0/2.0) * ( CiHQ1_11 + CiHQ1_22 ) / LambdaNP2
12073  +4218.6 * (1.0/2.0) * ( CiHu_11 + CiHu_22 ) / LambdaNP2
12074  +9648.28 * (1.0/2.0) * ( CiHQ3_11 + CiHQ3_22 ) / LambdaNP2
12075  -17762.5 * CiHD / LambdaNP2
12076  -13473.3 * CiHB / LambdaNP2
12077  -45667.9 * CiHW / LambdaNP2
12078  -110057. * CiHWB / LambdaNP2
12079  +16854.2 * CiDHB / LambdaNP2
12080  +30781.7 * CiDHW / LambdaNP2
12081  -2.6 * DeltaGF() );
12082 
12083 // Linear contribution from Higgs self-coupling
12084  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12085 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12086  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12087 
12088  // Add modifications due to small variations of the SM parameters
12089  //dwidth += cHSM * ( 0.0 );
12090 
12091  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12092  //dwidth += eHZZint + eHZZpar;
12093 
12094  return dwidth;
12095 
12096 }

◆ deltaGammaHZuuRatio2()

double NPSMEFTd6::deltaGammaHZuuRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z u u)\)/ \(\Gamma(H\to Z u u)_{\mathrm{SM}}\)

Definition at line 12098 of file NPSMEFTd6.cpp.

12099 {
12100  double dwidth = 0.0;
12101 
12102 
12103  //Contributions that are quadratic in the effective coefficients
12104  return ( dwidth );
12105 
12106 }

◆ deltaGammaHZvvRatio1()

double NPSMEFTd6::deltaGammaHZvvRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 11944 of file NPSMEFTd6.cpp.

11945 {
11946  double dwidth = 0.0;
11947 
11948  double C1 = 0.0083;
11949 
11950  dwidth = ( +121530. * CiHbox / LambdaNP2
11951  -7943.34 * (1.0/3.0) * ( CiHL1_11 + CiHL1_22 + CiHL1_33 ) / LambdaNP2
11952  +7943.34 * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
11953  -229.41 * CiHD / LambdaNP2
11954  -13535.2 * CiHB / LambdaNP2
11955  -45480.6 * CiHW / LambdaNP2
11956  -24891. * CiHWB / LambdaNP2
11957  +16833. * CiDHB / LambdaNP2
11958  +30597.6 * CiDHW / LambdaNP2
11959  -2. * DeltaGF() );
11960 
11961 // Linear contribution from Higgs self-coupling
11962  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11963 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11964  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11965 
11966  // Add modifications due to small variations of the SM parameters
11967  //dwidth += cHSM * ( 0.0 );
11968 
11969  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11970  //dwidth += eHZZint + eHZZpar;
11971 
11972  return dwidth;
11973 
11974 }

◆ deltaGammaHZvvRatio2()

double NPSMEFTd6::deltaGammaHZvvRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 11976 of file NPSMEFTd6.cpp.

11977 {
11978  double dwidth = 0.0;
11979 
11980 
11981  //Contributions that are quadratic in the effective coefficients
11982  return ( dwidth );
11983 
11984 }

◆ deltaGammaHZZ2e2muRatio1()

double NPSMEFTd6::deltaGammaHZZ2e2muRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 11819 of file NPSMEFTd6.cpp.

11820 {
11821  double dwidth = 0.0;
11822 
11823  double C1 = 0.0083;
11824 
11825  dwidth = ( +120836. * CiHbox / LambdaNP2
11826  +126374. * (1.0/2.0) * ( CiHL1_11 + CiHL1_22 ) / LambdaNP2
11827  -109064. * (1.0/2.0) * ( CiHe_11 + CiHe_22 ) / LambdaNP2
11828  +126374. * (1.0/2.0) * ( CiHL3_11 + CiHL3_22 ) / LambdaNP2
11829  -42370.4 * CiHD / LambdaNP2
11830  -14299. * CiHB / LambdaNP2
11831  -47298.2 * CiHW / LambdaNP2
11832  -83098.2 * CiHWB / LambdaNP2
11833  +16362.7 * CiDHB / LambdaNP2
11834  +29503.4 * CiDHW / LambdaNP2
11835  -3.378 * DeltaGF()
11836  -0.85 * deltaGzd6() );
11837 
11838 // Linear contribution from Higgs self-coupling
11839  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11840 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11841  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11842 
11843  // Add modifications due to small variations of the SM parameters
11844  dwidth += cHSM * ( -10.07 * deltaMz()
11845  +15.626 * deltaMh()
11846  -0.128 * deltaaMZ()
11847  +2.258 * deltaGmu() );
11848 
11849  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11850  dwidth += eHZZint + eHZZpar;
11851 
11852  return dwidth;
11853 
11854 }

◆ deltaGammaHZZ2e2muRatio2()

double NPSMEFTd6::deltaGammaHZZ2e2muRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 11856 of file NPSMEFTd6.cpp.

11857 {
11858  double dwidth = 0.0;
11859 
11860  //Contributions that are quadratic in the effective coefficients
11861  return ( dwidth );
11862 
11863 }

◆ deltaGammaHZZ4dRatio1()

double NPSMEFTd6::deltaGammaHZZ4dRatio1 ( ) const
inline

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 2523 of file NPSMEFTd6.h.

2524  {
2525  return 1.0;
2526  };

◆ deltaGammaHZZ4dRatio2()

double NPSMEFTd6::deltaGammaHZZ4dRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

◆ deltaGammaHZZ4eRatio1()

double NPSMEFTd6::deltaGammaHZZ4eRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 11756 of file NPSMEFTd6.cpp.

11757 {
11758  double dwidth = 0.0;
11759 
11760  double C1 = 0.0083;
11761 
11762  dwidth = ( +121386. * CiHbox / LambdaNP2
11763  +123413. * CiHL1_11 / LambdaNP2
11764  -103717. * CiHe_11 / LambdaNP2
11765  +123413. * CiHL3_11 / LambdaNP2
11766  -44056.9 * CiHD / LambdaNP2
11767  -13385.3 * CiHB / LambdaNP2
11768  -45127.7 * CiHW / LambdaNP2
11769  -91708.7 * CiHWB / LambdaNP2
11770  +16138.9 * CiDHB / LambdaNP2
11771  +28759.4 * CiDHW / LambdaNP2
11772  -3.462 * DeltaGF()
11773  -0.769 * deltaGzd6() );
11774 
11775 // Linear contribution from Higgs self-coupling
11776  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11777 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11778  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11779 
11780  // Add modifications due to small variations of the SM parameters
11781  dwidth += cHSM * ( -9.228 * deltaMz()
11782  +15.148 * deltaMh()
11783  -0.229 * deltaaMZ()
11784  +2.493 * deltaGmu() );
11785 
11786  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11787  dwidth += eHZZint + eHZZpar;
11788 
11789  return dwidth;
11790 
11791 }

◆ deltaGammaHZZ4eRatio2()

double NPSMEFTd6::deltaGammaHZZ4eRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 11793 of file NPSMEFTd6.cpp.

11794 {
11795  double dwidth = 0.0;
11796 
11797 
11798  //Contributions that are quadratic in the effective coefficients
11799  return ( dwidth );
11800 
11801 }

◆ deltaGammaHZZ4fRatio1()

double NPSMEFTd6::deltaGammaHZZ4fRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 12246 of file NPSMEFTd6.cpp.

12247 {
12248  double dwidth = 0.0;
12249 
12250  double C1 = 0.0083;
12251 
12252  double CZff, sf;
12253 
12254  CZff = gZvL*(-0.5 * (CiHL1_11 + CiHL1_22 + CiHL1_33 - CiHL3_11 - CiHL3_22 - CiHL3_33) * v2_over_LambdaNP2) +
12256  gZlR*(-0.5 * (CiHe_11 + CiHe_22 + CiHe_33) * v2_over_LambdaNP2) +
12257  Nc * (
12259  gZdR*(-0.5 * (CiHd_11 + CiHd_22 + CiHd_33) * v2_over_LambdaNP2) +
12261  gZuR*(-0.5 * (CiHu_11 + CiHu_22) * v2_over_LambdaNP2)
12262  );
12263 
12264  CZff = CZff/(
12265  3.0*( gZvL*gZvL + gZlL*gZlL + gZlR*gZlR ) +
12266  Nc * ( 3.0*( gZdL*gZdL + gZdR*gZdR ) + 2.0*( gZuL*gZuL + gZuR*gZuR ) )
12267  );
12268 
12269  sf = -11267.6 * (1.0/3.0) * (
12270  3.0*( gZvL*gZvL + gZlL*gZlL + gZlR*gZlR ) +
12271  Nc * ( 3.0*( gZdL*gZdL + gZdR*gZdR ) + 2.0*( gZuL*gZuL + gZuR*gZuR ) )
12272  );
12273 
12274  sf = sf/(-0.5*(gZlL + gZvL)*v2) ; // Coefficient of the CZff term. From the CiHL1_11 term in the ME.
12275 
12276  dwidth = ( +121373. * CiHbox / LambdaNP2
12277  + sf*CZff
12278  -50927.1 * CiHD / LambdaNP2
12279  -14137.9 * CiHB / LambdaNP2
12280  -46350.1 * CiHW / LambdaNP2
12281  -126336. * CiHWB / LambdaNP2
12282  +16558.7 * CiDHB / LambdaNP2
12283  +29628.7 * CiDHW / LambdaNP2
12284  -3.715 * DeltaGF()
12285  -0.834 * deltaGzd6()
12286  );
12287 
12288 // Linear contribution from Higgs self-coupling
12289  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12290 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12291  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12292 
12293  // Add modifications due to small variations of the SM parameters
12294  dwidth += cHSM * ( -9.548 * deltaMz()
12295  +15.799 * deltaMh()
12296  -0.412 * deltaaMZ()
12297  +2.569 * deltaGmu() );
12298 
12299  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12300  dwidth += eHZZint + eHZZpar;
12301 
12302  return dwidth;
12303 
12304 }

◆ deltaGammaHZZ4fRatio2()

double NPSMEFTd6::deltaGammaHZZ4fRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 12306 of file NPSMEFTd6.cpp.

12307 {
12308  double dwidth = 0.0;
12309 
12310 
12311  //Contributions that are quadratic in the effective coefficients
12312  return ( dwidth );
12313 
12314 }

◆ deltaGammaHZZ4lRatio1()

double NPSMEFTd6::deltaGammaHZZ4lRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 11686 of file NPSMEFTd6.cpp.

11687 {
11688  double dwidth = 0.0;
11689 
11690  double C1 = 0.0083;
11691 
11692  double CZll, sf;
11693 
11694  CZll = gZlL*(-0.5 * (CiHL1_11 + CiHL1_22 + CiHL3_11 + CiHL3_22) * v2_over_LambdaNP2) +
11695  gZlR*(-0.5 * (CiHe_11 + CiHe_22) * v2_over_LambdaNP2);
11696 
11697  CZll = CZll/(2.0*(gZlL*gZlL + gZlR*gZlR));
11698 
11699  sf = 124479. * (1.0/2.0) * (2.0*(gZlL*gZlL + gZlR*gZlR))/(-0.5*gZlL*v2) ; // Coefficient of the CZll term. From the CiHL1_11 term in the ME.
11700 
11701  dwidth = ( +122273. * CiHbox / LambdaNP2
11702  + sf*CZll
11703  -44025.7 * CiHD / LambdaNP2
11704  -13602.6 * CiHB / LambdaNP2
11705  -45248.6 * CiHW / LambdaNP2
11706  -88372.1 * CiHWB / LambdaNP2
11707  +16088.6 * CiDHB / LambdaNP2
11708  +29210.1 * CiDHW / LambdaNP2
11709  -3.462 * DeltaGF()
11710  -0.808 * deltaGzd6() );
11711 
11712 // Linear contribution from Higgs self-coupling
11713  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11714 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11715  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11716 
11717  // Add modifications due to small variations of the SM parameters
11718  dwidth += cHSM * ( -9.734 * deltaMz()
11719  +15.37 * deltaMh()
11720  -0.154 * deltaaMZ()
11721  +2.339 * deltaGmu() );
11722 
11723  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11724  dwidth += eHZZint + eHZZpar;
11725 
11726  return dwidth;
11727 
11728 }

◆ deltaGammaHZZ4lRatio2()

double NPSMEFTd6::deltaGammaHZZ4lRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 11730 of file NPSMEFTd6.cpp.

11731 {
11732  double dwidth = 0.0;
11733 
11734 
11735  //Contributions that are quadratic in the effective coefficients
11736  return ( dwidth );
11737 
11738 }

◆ deltaGammaHZZ4muRatio1()

double NPSMEFTd6::deltaGammaHZZ4muRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 11881 of file NPSMEFTd6.cpp.

11882 {
11883  double dwidth = 0.0;
11884 
11885  double C1 = 0.0083;
11886 
11887  dwidth = ( +120688. * CiHbox / LambdaNP2
11888  +123059. * CiHL1_22 / LambdaNP2
11889  -103862. * CiHe_22 / LambdaNP2
11890  +123059. * CiHL3_22 / LambdaNP2
11891  -43977.1 * CiHD / LambdaNP2
11892  -13575.5 * CiHB / LambdaNP2
11893  -45200.8 * CiHW / LambdaNP2
11894  -91625.2 * CiHWB / LambdaNP2
11895  +15449.3 * CiDHB / LambdaNP2
11896  +28489.5 * CiDHW / LambdaNP2
11897  -3.471 * DeltaGF()
11898  -0.774 * deltaGzd6() );
11899 
11900 // Linear contribution from Higgs self-coupling
11901  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11902 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11903  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11904 
11905  // Add modifications due to small variations of the SM parameters
11906  dwidth += cHSM * ( -9.254 * deltaMz()
11907  +15.109 * deltaMh()
11908  -0.207 * deltaaMZ()
11909  +2.405 * deltaGmu() );
11910 
11911  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11912  dwidth += eHZZint + eHZZpar;
11913 
11914  return dwidth;
11915 
11916 }

◆ deltaGammaHZZ4muRatio2()

double NPSMEFTd6::deltaGammaHZZ4muRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 11918 of file NPSMEFTd6.cpp.

11919 {
11920  double dwidth = 0.0;
11921 
11922 
11923  //Contributions that are quadratic in the effective coefficients
11924  return ( dwidth );
11925 
11926 }

◆ deltaGammaHZZ4uRatio1()

double NPSMEFTd6::deltaGammaHZZ4uRatio1 ( ) const
inline

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 u)\)/ \(\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

Definition at line 2506 of file NPSMEFTd6.h.

2507  {
2508  return 1.0;
2509  };

◆ deltaGammaHZZ4uRatio2()

double NPSMEFTd6::deltaGammaHZZ4uRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4 u)\)/ \(\Gamma(H\to ZZ* \to 4 u)_{\mathrm{SM}}\)

◆ deltaGammaHZZ4vRatio1()

double NPSMEFTd6::deltaGammaHZZ4vRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 12002 of file NPSMEFTd6.cpp.

12003 {
12004  double dwidth = 0.0;
12005 
12006  double C1 = 0.0083;
12007 
12008  dwidth = ( +120596. * CiHbox / LambdaNP2
12009  -115532. * (1.0/3.0) * ( CiHL1_11 + CiHL1_22 + CiHL1_33 ) / LambdaNP2
12010  +115532. * (1.0/3.0) * ( CiHL3_11 + CiHL3_22 + CiHL3_33 ) / LambdaNP2
12011  -28744.1 * CiHD / LambdaNP2
12012  -13816.7 * CiHB / LambdaNP2
12013  -44782.1 * CiHW / LambdaNP2
12014  -25256.6 * CiHWB / LambdaNP2
12015  +15982.5 * CiDHB / LambdaNP2
12016  +28910.7 * CiDHW / LambdaNP2
12017  -3.013 * DeltaGF()
12018  -0.787 * deltaGzd6()
12019  );
12020 
12021 // Linear contribution from Higgs self-coupling
12022  dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
12023 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
12024  dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
12025 
12026  // Add modifications due to small variations of the SM parameters
12027  dwidth += cHSM * ( -10.49 * deltaMz()
12028  +15.294 * deltaMh()
12029  +0.255 * deltaaMZ()
12030  +1.979 * deltaGmu() );
12031 
12032  // SM (1) + intrinsic + parametric theory relative errors (free pars)
12033  dwidth += eHZZint + eHZZpar;
12034 
12035  return dwidth;
12036 
12037 }

◆ deltaGammaHZZ4vRatio2()

double NPSMEFTd6::deltaGammaHZZ4vRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 12039 of file NPSMEFTd6.cpp.

12040 {
12041  double dwidth = 0.0;
12042 
12043 
12044  //Contributions that are quadratic in the effective coefficients
12045  return ( dwidth );
12046 
12047 }

◆ deltaGammaHZZRatio1()

double NPSMEFTd6::deltaGammaHZZRatio1 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 11457 of file NPSMEFTd6.cpp.

11458 {
11459  double dwidth = 0.0;
11460 
11461 // double C1 = 0.0083;
11462 
11463  dwidth = deltaGammaHZZ4fRatio1();
11464 
11465 // Linear contribution from Higgs self-coupling
11466 // dwidth = dwidth + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
11467 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
11468 // dwidth = dwidth + cLHd6*cLH3d62*dZH*deltaG_hhhRatio()*deltaG_hhhRatio();
11469 
11470  // SM (1) + intrinsic + parametric theory relative errors (free pars)
11471 // dwidth += eHZZint + eHZZpar;
11472 
11473  return dwidth;
11474 
11475 }

◆ deltaGammaHZZRatio2()

double NPSMEFTd6::deltaGammaHZZRatio2 ( ) const

The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)

Returns
\(\delta \Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 11477 of file NPSMEFTd6.cpp.

11478 {
11479  double dwidth = 0.0;
11480 
11481  //Contributions that are quadratic in the effective coefficients
11482  dwidth = deltaGammaHZZ4fRatio2();
11483 
11484 
11485  return dwidth;
11486 
11487 }

◆ deltaGammaTotalRatio1()

double NPSMEFTd6::deltaGammaTotalRatio1 ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 10909 of file NPSMEFTd6.cpp.

10910 {
10911  double deltaGammaRatio;
10912 
10913 // The change in the ratio asumming only SM decays
10914  deltaGammaRatio = ( trueSM.computeBrHtogg() * deltaGammaHggRatio1()
10923 
10924 // Add the effect of the invisible and exotic BR. Include also here the
10925 // pure contribution from BrHinv and BrHexo even in case of no dim 6 contibutions
10926  deltaGammaRatio = -1.0 + (1.0 + deltaGammaRatio) / (1.0 - BrHinv - BrHexo);
10927 
10928  return deltaGammaRatio;
10929 }

◆ deltaGammaTotalRatio1noError()

double NPSMEFTd6::deltaGammaTotalRatio1noError ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 10931 of file NPSMEFTd6.cpp.

10932 {
10933  double deltaGammaRatio;
10934 
10935 // The change in the ratio asumming only SM decays
10936  deltaGammaRatio = ( trueSM.computeBrHtogg() * (deltaGammaHggRatio1() - eHggint - eHggpar )
10945 
10946 // Add the effect of the invisible and exotic BR. Include also here the
10947 // pure contribution from BrHinv and BrHexo even in case of no dim 6 contibutions
10948  deltaGammaRatio = -1.0 + (1.0 + deltaGammaRatio) / (1.0 - BrHinv - BrHexo);
10949 
10950  return deltaGammaRatio;
10951 }

◆ deltaGammaTotalRatio2()

double NPSMEFTd6::deltaGammaTotalRatio2 ( ) const
virtual

The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.

Returns
\(\delta \Gamma(H)\)/ \(\Gamma(H)_{\mathrm{SM}}\)

Definition at line 10953 of file NPSMEFTd6.cpp.

10954 {
10955  double deltaGammaRatio;
10956 
10957 // The change in the ratio asumming only SM decays
10958  deltaGammaRatio = trueSM.computeBrHtogg() * deltaGammaHggRatio2()
10967 
10968 // Add the effect of the invisible and exotic BR and return
10969  return (deltaGammaRatio / (1.0 - BrHinv - BrHexo));
10970 }

◆ DeltaGF()

double NPSMEFTd6::DeltaGF ( ) const
virtual

New physics contribution to the Fermi constant.

The new physics contribution \(\Delta G\) is defined as

\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]

where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.

Returns
\(\Delta G\)

Reimplemented from NPbase.

Definition at line 2922 of file NPSMEFTd6.cpp.

2923 {
2924  return ((CiHL3_11 + CiHL3_22 - 0.5 * (CiLL_1221 + CiLL_2112)) * v2_over_LambdaNP2);
2925 }

◆ deltaGL_f()

double NPSMEFTd6::deltaGL_f ( const Particle  p) const

New physics contribution to the neutral-current left-handed coupling \(g_L^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_L^f\)

Definition at line 3176 of file NPSMEFTd6.cpp.

3177 {
3178  double I3p = p.getIsospin(), Qp = p.getCharge();
3179  double CHF1 = CHF1_diag(p);
3180  double CHF3 = CHF3_diag(p);
3181  double NPindirect;
3182 
3183  NPindirect = -I3p / 4.0 * (CiHD * v2_over_LambdaNP2 + 2.0 * DeltaGF())
3184  - Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
3185  *((4.0 * cW_tree / sW_tree * CiHWB + CiHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
3186 
3187  double NPdirect = -0.5 * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2;
3188  return (NPindirect + NPdirect);
3189 }

◆ deltaGL_Wff()

gslpp::complex NPSMEFTd6::deltaGL_Wff ( const Particle  pbar,
const Particle  p 
) const
virtual

New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{Wff}^{L}\)

Reimplemented from NPbase.

Definition at line 3207 of file NPSMEFTd6.cpp.

3208 {
3209  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
3210  throw std::runtime_error("NPSMEFTd6::deltaGL_Wff(): Not implemented");
3211 
3212  double CHF3 = CHF3_diag(pbar);
3213  double NPindirect;
3214 
3215  NPindirect = -cW2_tree / 4.0 / (cW2_tree - sW2_tree)
3216  * ((4.0 * sW_tree / cW_tree * CiHWB + CiHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
3217 
3218  double NPdirect = CHF3 * v2_over_LambdaNP2;
3219  return (NPindirect + NPdirect);
3220 }

◆ deltaGL_Wffh()

gslpp::complex NPSMEFTd6::deltaGL_Wffh ( const Particle  pbar,
const Particle  p 
) const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{WffH}^{L}\)

Definition at line 3467 of file NPSMEFTd6.cpp.

3468 {
3469  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
3470  throw std::runtime_error("NPSMEFTd6::deltaGL_Wffh(): Not implemented");
3471 
3472  double CHF3 = CHF3_diag(pbar);
3473  return (2.0 * sqrt(2.0) * Mz * cW_tree / v() / v() * CHF3 * v2_over_LambdaNP2);
3474 }

◆ deltaGL_Zffh()

double NPSMEFTd6::deltaGL_Zffh ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{ZffH}^{L}\)

Definition at line 3485 of file NPSMEFTd6.cpp.

3486 {
3487  double I3p = p.getIsospin();
3488  double CHF1 = CHF1_diag(p);
3489  double CHF3 = CHF3_diag(p);
3490  return (-2.0 * Mz / v() / v() * (CHF1 - 2.0 * I3p * CHF3) * v2_over_LambdaNP2);
3491 }

◆ deltaGmu()

double NPSMEFTd6::deltaGmu ( ) const
virtual

The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta G_\mu/G_\mu\)

Definition at line 3020 of file NPSMEFTd6.cpp.

3021 {
3022  // Ref. value fixed in SM EW fit 2018: from PDG 2018
3023  return ( (GF - 1.1663787/100000.0 ) / (1.1663787/100000.0) );
3024 }

◆ deltaGmu2()

double NPSMEFTd6::deltaGmu2 ( ) const
virtual

The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta G_\mu/G_\mu)^2\)

Definition at line 3026 of file NPSMEFTd6.cpp.

3027 {
3028  return ( 0.0 );
3029 }

◆ deltaGR_f()

double NPSMEFTd6::deltaGR_f ( const Particle  p) const

New physics contribution to the neutral-current right-handed coupling \(g_R^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_R^f\)

Definition at line 3191 of file NPSMEFTd6.cpp.

3192 {
3193  double Qp = p.getCharge();
3194  double CHf = CHf_diag(p);
3195  double NPindirect;
3196 
3197  NPindirect = -Qp * sW2_tree / 4.0 / (cW2_tree - sW2_tree)
3198  *((4.0 * cW_tree / sW_tree * CiHWB + CiHD) * v2_over_LambdaNP2 + 2.0 * DeltaGF());
3199 
3200  double NPdirect = -0.5 * CHf*v2_over_LambdaNP2;
3201  return (NPindirect + NPdirect);
3202 }

◆ deltaGR_Wff()

gslpp::complex NPSMEFTd6::deltaGR_Wff ( const Particle  pbar,
const Particle  p 
) const
virtual

New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{Wff}^{R}\)

Reimplemented from NPbase.

Definition at line 3222 of file NPSMEFTd6.cpp.

3223 {
3224  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
3225  throw std::runtime_error("NPSMEFTd6::deltaGR_Wff(): Not implemented");
3226 
3227  gslpp::complex CHud = CHud_diag(pbar);
3228  return (0.5 * CHud * v2_over_LambdaNP2);
3229 }

◆ deltaGR_Wffh()

gslpp::complex NPSMEFTd6::deltaGR_Wffh ( const Particle  pbar,
const Particle  p 
) const

The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pbara lepton or quark
[in]pa lepton or quark
Returns
\(\delta g_{WffH}^{R}\)

Definition at line 3476 of file NPSMEFTd6.cpp.

3477 {
3478  if (pbar.getIndex() + 1 != p.getIndex() || pbar.getIndex() % 2 != 0)
3479  throw std::runtime_error("NPSMEFTd6::deltaGR_Wffh(): Not implemented");
3480 
3481  gslpp::complex CHud = CHud_diag(pbar);
3482  return (sqrt(2.0) * Mz * cW_tree / v() / v() * CHud * v2_over_LambdaNP2);
3483 }

◆ deltaGR_Zffh()

double NPSMEFTd6::deltaGR_Zffh ( const Particle  p) const

The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).

Parameters
[in]pa lepton or quark
Returns
\(\delta g_{ZffH}^{R}\)

Definition at line 3493 of file NPSMEFTd6.cpp.

3494 {
3495  double CHf = CHf_diag(p);
3496  return (-2.0 * Mz / v() / v() * CHf * v2_over_LambdaNP2);
3497 }

◆ deltaGV_f()

double NPSMEFTd6::deltaGV_f ( const Particle  p) const
virtual

New physics contribution to the neutral-current vector coupling \(g_V^f\).

Parameters
[in]fa lepton or quark
Returns
\(\delta g_V^f\)

Reimplemented from NPbase.

Definition at line 3166 of file NPSMEFTd6.cpp.

3167 {
3168  return (deltaGL_f(p) + deltaGR_f(p));
3169 }

◆ deltaGwd6()

double NPSMEFTd6::deltaGwd6 ( ) const
virtual

The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\).

Returns
\(\delta \Gamma_W/\Gamma_W\)

Definition at line 3142 of file NPSMEFTd6.cpp.

3143 {
3144  return ( deltaGamma_W() / trueSM.GammaW() );
3145 }

◆ deltaGwd62()

double NPSMEFTd6::deltaGwd62 ( ) const
virtual

The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\).

Returns
\((\delta \Gamma_W/\Gamma_W)^2\)

Definition at line 3147 of file NPSMEFTd6.cpp.

3148 {
3149  double dWW = 0.0;
3150 
3151  return (dWW*dWW);
3152 }

◆ deltaGzd6()

double NPSMEFTd6::deltaGzd6 ( ) const
virtual

The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\).

Returns
\(\delta \Gamma_Z/\Gamma_Z\)

Definition at line 3154 of file NPSMEFTd6.cpp.

3155 {
3156  return ( deltaGamma_Z() / trueSM.Gamma_Z() );
3157 }

◆ deltaGzd62()

double NPSMEFTd6::deltaGzd62 ( ) const
virtual

The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\).

Returns
\((\delta \Gamma_Z/\Gamma_Z)^2\)

Definition at line 3159 of file NPSMEFTd6.cpp.

3160 {
3161  double dWZ = 0.0;
3162 
3163  return (dWZ*dWZ);
3164 }

◆ deltaKgammaNP()

double NPSMEFTd6::deltaKgammaNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).

Returns
\(\delta \kappa_{\gamma}\)

Reimplemented from NPbase.

Definition at line 13836 of file NPSMEFTd6.cpp.

13837 {
13838  double NPdirect;
13839 
13840  /* Translate from LHCHXWG-INT-2015-001: Checked with own calculations */
13841  NPdirect = sqrt( 4.0 * M_PI * aleMz ) / 4.0 / sW2_tree;
13842 
13843  NPdirect = NPdirect * ( (4.0 * sW_tree * cW_tree / sqrt( 4.0 * M_PI * aleMz ) ) * CiHWB
13844  - sW_tree * CiDHW
13846 
13847  return NPdirect + dKappaga ;
13848 }

◆ deltaKgammaNPEff()

double NPSMEFTd6::deltaKgammaNPEff ( ) const
virtual

The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph].

Returns
\(\delta \kappa_{\gamma}\)

Reimplemented from NPbase.

Definition at line 13875 of file NPSMEFTd6.cpp.

13876 {
13877  /* From arXiv:1708.09079 [hep-ph]. In our case, delta_e=0 since it is taken as inputs and its effects propagated
13878  * everywhere else */
13879  double dgEff;
13880 
13883 
13884  return dgEff + deltaKgammaNP() ;
13885 }

◆ deltamb()

double NPSMEFTd6::deltamb ( ) const
virtual

The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_b/m_b\)

Definition at line 2987 of file NPSMEFTd6.cpp.

2988 {
2989  // Ref. value fixed in SM EW fit 2018: from PDG 2018
2990  return ( ((quarks[BOTTOM].getMass()) - 4.18) / 4.18 );
2991 }

◆ deltamb2()

double NPSMEFTd6::deltamb2 ( ) const
virtual

The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_b/m_b)^2\)

Definition at line 2993 of file NPSMEFTd6.cpp.

2994 {
2995  return ( 0.0 );
2996 }

◆ deltamc()

double NPSMEFTd6::deltamc ( ) const
virtual

The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_c/m_c\)

Definition at line 2998 of file NPSMEFTd6.cpp.

2999 {
3000  // Ref. value fixed in SM EW fit 2018: from PDG 2018
3001  return ( ((quarks[CHARM].getMass()) - 1.275) / 1.275 );
3002 }

◆ deltamc2()

double NPSMEFTd6::deltamc2 ( ) const
virtual

The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_c/m_c)^2\)

Definition at line 3004 of file NPSMEFTd6.cpp.

3005 {
3006  return ( 0.0 );
3007 }

◆ deltaMh()

double NPSMEFTd6::deltaMh ( ) const
virtual

The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta M_H/M_H\)

Definition at line 2965 of file NPSMEFTd6.cpp.

2966 {
2967  // Ref. value from SM EW fit 2018
2968  return ( (mHl - 125.1) / 125.1 );
2969 }

◆ deltaMh2()

double NPSMEFTd6::deltaMh2 ( ) const
virtual

The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta M_H/M_H)^2\)

Definition at line 2971 of file NPSMEFTd6.cpp.

2972 {
2973  return ( 0.0 );
2974 }

◆ deltamt()

double NPSMEFTd6::deltamt ( ) const
virtual

The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_t/m_t\)

Definition at line 2976 of file NPSMEFTd6.cpp.

2977 {
2978  // Ref. value from SM EW fit 2018
2979  return ( (mtpole - 173.2) / 173.2 );
2980 }

◆ deltamt2()

double NPSMEFTd6::deltamt2 ( ) const
virtual

The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_t/m_t)^2\)

Definition at line 2982 of file NPSMEFTd6.cpp.

2983 {
2984  return ( 0.0 );
2985 }

◆ deltamtau()

double NPSMEFTd6::deltamtau ( ) const
virtual

The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta m_\tau/m_\tau\)

Definition at line 3009 of file NPSMEFTd6.cpp.

3010 {
3011  // Ref. value fixed in SM EW fit 2018: from PDG 2018
3012  return ( ((leptons[TAU].getMass()) - 1.77686) / 1.77686 );
3013 }

◆ deltamtau2()

double NPSMEFTd6::deltamtau2 ( ) const
virtual

The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta m_\tau/m_\tau)^2\)

Definition at line 3015 of file NPSMEFTd6.cpp.

3016 {
3017  return ( 0.0 );
3018 }

◆ deltaMwd6()

double NPSMEFTd6::deltaMwd6 ( ) const
virtual

The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\).

Returns
\(\delta M_W/M_W\)

Definition at line 3075 of file NPSMEFTd6.cpp.

3076 {
3077  return (- 1.0 / 4.0 / (cW2_tree - sW2_tree)
3078  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
3080  + 2.0 * sW2_tree * DeltaGF()));
3081 }

◆ deltaMwd62()

double NPSMEFTd6::deltaMwd62 ( ) const
virtual

The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\).

Returns
\((\delta M_W/M_W)^2\)

Definition at line 3083 of file NPSMEFTd6.cpp.

3084 {
3085  double dMW = 0.0;
3086 
3087  return (dMW*dMW);
3088 }

◆ deltaMz()

double NPSMEFTd6::deltaMz ( ) const
virtual

The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\(\delta M_Z/M_Z\)

Definition at line 2954 of file NPSMEFTd6.cpp.

2955 {
2956  // Ref. value from SM EW fit 2018
2957  return ( (Mz - 91.1882) / 91.1882 );
2958 }

◆ deltaMz2()

double NPSMEFTd6::deltaMz2 ( ) const
virtual

The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables.

Returns
\((\delta M_Z/M_Z)^2\)

Definition at line 2960 of file NPSMEFTd6.cpp.

2961 {
2962  return ( 0.0 );
2963 }

◆ deltayb_HB()

double NPSMEFTd6::deltayb_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_b\)

Reimplemented from NPbase.

Definition at line 15480 of file NPSMEFTd6.cpp.

15481 {
15482  double mf= (quarks[BOTTOM].getMass());
15483  double ciHB;
15484 
15485  ciHB = - (v()/mf/sqrt(2.0))*CidH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15486 
15487  return ciHB;
15488 }

◆ deltayc_HB()

double NPSMEFTd6::deltayc_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_c\)

Reimplemented from NPbase.

Definition at line 15502 of file NPSMEFTd6.cpp.

15503 {
15504  double mf= (quarks[CHARM].getMass());
15505  double ciHB;
15506 
15507  ciHB = - (v()/mf/sqrt(2.0))*CiuH_22r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15508 
15509  return ciHB;
15510 }

◆ deltaymu_HB()

double NPSMEFTd6::deltaymu_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_\mu\)

Reimplemented from NPbase.

Definition at line 15513 of file NPSMEFTd6.cpp.

15514 {
15515  double mf= (leptons[MU].getMass());
15516  double ciHB;
15517 
15518  ciHB = - (v()/mf/sqrt(2.0))*CieH_22r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15519 
15520  return ciHB;
15521 }

◆ deltayt_HB()

double NPSMEFTd6::deltayt_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_t\)

Reimplemented from NPbase.

Definition at line 15469 of file NPSMEFTd6.cpp.

15470 {
15471  double mf= mtpole;
15472  double ciHB;
15473 
15474  ciHB = - (v()/mf/sqrt(2.0))*CiuH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15475 
15476  return ciHB;
15477 }

◆ deltaytau_HB()

double NPSMEFTd6::deltaytau_HB ( ) const
virtual

The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\delta y_\tau\)

Reimplemented from NPbase.

Definition at line 15491 of file NPSMEFTd6.cpp.

15492 {
15493  double mf= (leptons[TAU].getMass());
15494  double ciHB;
15495 
15496  ciHB = - (v()/mf/sqrt(2.0))*CieH_33r*v2_over_LambdaNP2 + delta_h - 0.5*DeltaGF();
15497 
15498  return ciHB;
15499 }

◆ dxseeWWdcos()

double NPSMEFTd6::dxseeWWdcos ( const double  sqrt_s,
const double  cos 
) const
virtual

The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.

Returns
\(d\sigma/d\cos{\theta}\)

Reimplemented from NPbase.

Definition at line 13889 of file NPSMEFTd6.cpp.

13890 {
13891  double sqrt_sGeV = 1000. * sqrt_s;
13892  double s = sqrt_sGeV * sqrt_sGeV;
13893  double cos2 = cos * cos;
13894  double sin2 = 1.0 - cos2;
13895  double sin = sqrt(sin2);
13896 
13897  double topb = 0.3894*1000000000.0;
13898 
13899 // NC and CC couplings
13900  double gLe, gRe;
13901  gslpp::complex Uenu;
13902 
13903  gLe = -0.5 + sW2_tree + deltaGL_f(leptons[ELECTRON]);
13904  gRe = sW2_tree + deltaGR_f(leptons[ELECTRON]);
13905 
13907  Uenu = 1.0 + Uenu;
13908 
13909 // W mass
13910  double mw;
13911 
13912  mw = Mw();
13913 
13914 // Wigner functions
13915  double d1pp[2],d1mm[2],d1p0[2],d1m0[2],d10p[2],d10m[2],d100[2];
13916 
13917  d1pp[0]=sqrt((1.0 - cos2)/2.0);
13918  d1pp[1]=-sqrt((1.0 - cos2)/2.0);
13919 
13920  d1mm[0]=d1pp[0];
13921  d1mm[1]=d1pp[1];
13922 
13923  d1p0[0]=(1.0 - cos)/2.0;
13924  d1p0[1]=(1.0 + cos)/2.0;
13925 
13926  d1m0[0]=d1p0[1];
13927  d1m0[1]=d1p0[0];
13928 
13929  d10p[0]=d1p0[1];
13930  d10p[1]=d1p0[0];
13931 
13932  d10m[0]=d1p0[0];
13933  d10m[1]=d1p0[1];
13934 
13935  d100[0]=d1pp[0];
13936  d100[1]=d1pp[1];
13937 
13938  gslpp::matrix<double> d1LH(3, 3, 0.0);
13939 
13940  gslpp::matrix<double> d1RH(3, 3, 0.0);
13941 
13942  d1LH.assign(0,0, d1pp[0]);
13943  d1LH.assign(0,1, d1p0[0]);
13944  d1LH.assign(0,2, 0.0);
13945 
13946  d1LH.assign(1,0, d10p[0]);
13947  d1LH.assign(1,1, d100[0]);
13948  d1LH.assign(1,2, d10m[0]);
13949 
13950  d1LH.assign(2,0, 0.0);
13951  d1LH.assign(2,1, d1m0[0]);
13952  d1LH.assign(2,2, d1mm[0]);
13953 
13954  d1RH.assign(0,0, d1pp[1]);
13955  d1RH.assign(0,1, d1p0[1]);
13956  d1RH.assign(0,2, 0.0);
13957 
13958  d1RH.assign(1,0, d10p[1]);
13959  d1RH.assign(1,1, d100[1]);
13960  d1RH.assign(1,2, d10m[1]);
13961 
13962  d1RH.assign(2,0, 0.0);
13963  d1RH.assign(2,1, d1m0[1]);
13964  d1RH.assign(2,2, d1mm[1]);
13965 
13966 // TGC parameterization
13967  double g1Z,g1ga,kZ,kga,lambdaZ,lambdaga,g4Z,g4ga,g5Z,g5ga,ktZ,ktga,lambdatZ,lambdatga;
13968 
13969 // TGC present in the SM
13970  g1Z=1.0 + deltag1ZNP();
13971  g1ga=1.0;
13972  kZ=1.0 + deltag1ZNP() - (sW2_tree/cW2_tree) * deltaKgammaNP();
13973  kga=1.0 + deltaKgammaNP();
13974 // TGC not present in the SM
13975  lambdaZ=lambdaZNP(); //Check normalization
13976  lambdaga=lambdaZ;
13977  g4Z=0.0;
13978  g4ga=0.0;
13979  g5Z=0.0;
13980  g5ga=0.0;
13981  ktZ=0.0;
13982  ktga=0.0;
13983  lambdatZ=0.0;
13984  lambdatga=0.0;
13985 
13986  double f3Z, f3ga;
13987 
13988  f3Z = g1Z + kZ + lambdaZ;
13989  f3ga = g1ga + kga + lambdaga;
13990 
13991  // Kinematic factors
13992  double beta, gamma, gamma2;
13993 
13994  beta = sqrt(1.0 - 4.0 * mw * mw / s);
13995  gamma = sqrt_sGeV/(2.0 * mw);
13996  gamma2= gamma*gamma;
13997 
13998 // J=1 Subamplitudes: Z
13999  gslpp::complex AZpp, AZmm, AZp0, AZm0, AZ0p, AZ0m, AZ00;
14000 
14001  AZpp = gslpp::complex(g1Z + 2.0* gamma2* lambdaZ, (ktZ + lambdatZ - 2.0*lambdatZ)/beta , false);
14002  AZmm = gslpp::complex(g1Z + 2.0* gamma2* lambdaZ, -(ktZ + lambdatZ - 2.0*lambdatZ)/beta , false);
14003  AZp0 = gslpp::complex(f3Z + beta * g5Z , -g4Z + (ktZ-lambdatZ)/beta , false);
14004  AZp0 = gamma * AZp0;
14005  AZm0 = gslpp::complex(f3Z - beta * g5Z , -g4Z - (ktZ-lambdatZ)/beta , false);
14006  AZm0 = gamma * AZm0;
14007  AZ0p = gslpp::complex(f3Z - beta * g5Z , g4Z + (ktZ-lambdatZ)/beta , false);
14008  AZ0p = gamma * AZ0p;
14009  AZ0m = gslpp::complex(f3Z + beta * g5Z , g4Z - (ktZ-lambdatZ)/beta , false);
14010  AZ0m = gamma * AZ0m;
14011  AZ00 = gslpp::complex( g1Z + 2.0*gamma2*kZ, 0.0 , false);
14012 
14013 // Collect in matrices and separate LH and RH
14014  gslpp::matrix<gslpp::complex> AmpZLH(3, 3, 0.0);
14015  gslpp::matrix<gslpp::complex> AmpZRH(3, 3, 0.0);
14016 
14017  AmpZLH.assign(0,0, AZpp * d1LH(0,0) );
14018  AmpZLH.assign(0,1, AZp0 * d1LH(0,1));
14019  AmpZLH.assign(0,2, 0.0);
14020 
14021  AmpZLH.assign(1,0, AZ0p * d1LH(1,0));
14022  AmpZLH.assign(1,1, AZ00 * d1LH(1,1));
14023  AmpZLH.assign(1,2, AZ0m * d1LH(1,2));
14024 
14025  AmpZLH.assign(2,0, 0.0);
14026  AmpZLH.assign(2,1, AZm0 * d1LH(2,1));
14027  AmpZLH.assign(2,2, AZmm * d1LH(2,2));
14028 
14029  AmpZLH = AmpZLH * beta * s/(s-Mz*Mz);
14030 
14031 // Add the correct Zff coupling
14032  AmpZLH = AmpZLH * gLe / sW2_tree;
14033 
14034  AmpZRH.assign(0,0, AZpp * d1RH(0,0) );
14035  AmpZRH.assign(0,1, AZp0 * d1RH(0,1));
14036  AmpZRH.assign(0,2, 0.0);
14037 
14038  AmpZRH.assign(1,0, AZ0p * d1RH(1,0));
14039  AmpZRH.assign(1,1, AZ00 * d1RH(1,1));
14040  AmpZRH.assign(1,2, AZ0m * d1RH(1,2));
14041 
14042  AmpZRH.assign(2,0, 0.0);
14043  AmpZRH.assign(2,1, AZm0 * d1RH(2,1));
14044  AmpZRH.assign(2,2, AZmm * d1RH(2,2));
14045 
14046  AmpZRH = AmpZRH * beta * s/(s-Mz*Mz);
14047 
14048 // Add the correct Zff coupling
14049  AmpZRH = AmpZRH * gRe / sW2_tree;
14050 
14051 // J=1 Subamplitudes: gamma
14052  gslpp::complex Agapp, Agamm, Agap0, Agam0, Aga0p, Aga0m, Aga00;
14053 
14054  Agapp = gslpp::complex(g1ga + 2.0* gamma2* lambdaga, (ktga + lambdatga - 2.0*lambdatga)/beta , false);
14055  Agamm = gslpp::complex(g1ga + 2.0* gamma2* lambdaga, -(ktga + lambdatga - 2.0*lambdatga)/beta , false);
14056  Agap0 = gslpp::complex(f3ga + beta * g5ga , -g4ga + (ktga-lambdatga)/beta , false);
14057  Agap0 = gamma * Agap0;
14058  Agam0 = gslpp::complex(f3ga - beta * g5ga , -g4ga - (ktga-lambdatga)/beta , false);
14059  Agam0 = gamma * Agam0;
14060  Aga0p = gslpp::complex(f3ga - beta * g5ga , g4ga + (ktga-lambdatga)/beta , false);
14061  Aga0p = gamma * Aga0p;
14062  Aga0m = gslpp::complex(f3ga + beta * g5ga , g4ga - (ktga-lambdatga)/beta , false);
14063  Aga0m = gamma * Aga0m;
14064  Aga00 = gslpp::complex( g1ga + 2.0*gamma2*kga, 0.0 , false);
14065 
14066 // Collect in matrices. Here LH = RH, except for the Wigner functions
14067  gslpp::matrix<gslpp::complex> AmpgaLH(3, 3, 0.0);
14068  gslpp::matrix<gslpp::complex> AmpgaRH(3, 3, 0.0);
14069 
14070  AmpgaLH.assign(0,0, Agapp * d1LH(0,0));
14071  AmpgaLH.assign(0,1, Agap0 * d1LH(0,1));
14072  AmpgaLH.assign(0,2, 0.0);
14073 
14074  AmpgaLH.assign(1,0, Aga0p * d1LH(1,0));
14075  AmpgaLH.assign(1,1, Aga00 * d1LH(1,1));
14076  AmpgaLH.assign(1,2, Aga0m * d1LH(1,2));
14077 
14078  AmpgaLH.assign(2,0, 0.0);
14079  AmpgaLH.assign(2,1, Agam0 * d1LH(2,1));
14080  AmpgaLH.assign(2,2, Agamm * d1LH(2,2));
14081 
14082  AmpgaRH.assign(0,0, Agapp * d1RH(0,0));
14083  AmpgaRH.assign(0,1, Agap0 * d1RH(0,1));
14084  AmpgaRH.assign(0,2, 0.0);
14085 
14086  AmpgaRH.assign(1,0, Aga0p * d1RH(1,0));
14087  AmpgaRH.assign(1,1, Aga00 * d1RH(1,1));
14088  AmpgaRH.assign(1,2, Aga0m * d1RH(1,2));
14089 
14090  AmpgaRH.assign(2,0, 0.0);
14091  AmpgaRH.assign(2,1, Agam0 * d1RH(2,1));
14092  AmpgaRH.assign(2,2, Agamm * d1RH(2,2));
14093 
14094  AmpgaLH = -beta * AmpgaLH;
14095  AmpgaRH = -beta * AmpgaRH;
14096 
14097 // J=1 Subamplitudes: neutrino
14098  gslpp::complex Bpp, Bmm, Bp0, Bm0, B0p, B0m, B00;
14099  gslpp::complex Cpp, Cmm, Cp0, Cm0, C0p, C0m, C00;
14100 
14101  Bpp = gslpp::complex(1.0 , 0.0 , false);
14102  Bmm = Bpp;
14103  Bp0 = gslpp::complex( 2.0 * gamma, 0.0 , false);
14104  Bm0 = Bp0;
14105  B0p = Bp0;
14106  B0m = Bp0;
14107  B00 = gslpp::complex( 2.0 * gamma2, 0.0 , false);
14108 
14109  Cpp = gslpp::complex(1.0/gamma2 , 0.0 , false);
14110  Cmm = Cpp;
14111  Cp0 = gslpp::complex( 2.0 * (1.0 + beta)/gamma, 0.0 , false);
14112  Cm0 = gslpp::complex( 2.0 * (1.0 - beta)/gamma, 0.0 , false);
14113  C0p = Cm0;
14114  C0m = Cp0;
14115  C00 = gslpp::complex( 2.0 / gamma2, 0.0 , false);
14116 
14117 // Collect in matrices. Here LH = RH
14118  gslpp::matrix<gslpp::complex> Bnu(3, 3, 0.0);
14119  gslpp::matrix<gslpp::complex> Cnu(3, 3, 0.0);
14120 
14121  Bnu.assign(0,0, Bpp * d1LH(0,0));
14122  Bnu.assign(0,1, Bp0 * d1LH(0,1));
14123  Bnu.assign(0,2, 0.0);
14124 
14125  Bnu.assign(1,0, B0p * d1LH(1,0));
14126  Bnu.assign(1,1, B00 * d1LH(1,1));
14127  Bnu.assign(1,2, B0m * d1LH(1,2));
14128 
14129  Bnu.assign(2,0, 0.0);
14130  Bnu.assign(2,1, Bm0 * d1LH(2,1));
14131  Bnu.assign(2,2, Bmm * d1LH(2,2));
14132 
14133  Cnu.assign(0,0, Cpp * d1LH(0,0));
14134  Cnu.assign(0,1, Cp0 * d1LH(0,1));
14135  Cnu.assign(0,2, 0.0);
14136 
14137  Cnu.assign(1,0, C0p * d1LH(1,0));
14138  Cnu.assign(1,1, C00 * d1LH(1,1));
14139  Cnu.assign(1,2, C0m * d1LH(1,2));
14140 
14141  Cnu.assign(2,0, 0.0);
14142  Cnu.assign(2,1, Cm0 * d1LH(2,1));
14143  Cnu.assign(2,2, Cmm * d1LH(2,2));
14144 
14145 // The matrix with the total J=1 neutrino amplitude (only LH neutrinos)
14146  gslpp::matrix<gslpp::complex> Ampnu1(3, 3, 0.0);
14147 
14148  Ampnu1 = Bnu - Cnu/(1.0 + beta*beta - 2.0 * beta * cos);
14149 
14150  Ampnu1 = Uenu * Uenu.conjugate() * Ampnu1 / (2.0 * beta * sW2_tree);
14151 
14152  gslpp::matrix<gslpp::complex> Ampnu2(3, 3, 0.0);
14153 
14154  Ampnu2.assign(0,2, (1.0 - cos)/2.0 );
14155  Ampnu2.assign(1,1, 0.0);
14156  Ampnu2.assign(2,0, -(1.0 + cos)/2.0);
14157 
14158  Ampnu2 = (8.0 * M_PI * aleMz / sW2_tree)* Uenu * Uenu.conjugate() * Ampnu2 * sin / (1.0 + beta*beta - 2.0*beta*cos);
14159 
14160 // Total amplitudes
14161  gslpp::matrix<gslpp::complex> MRH(3, 3, 0.0);
14162  gslpp::matrix<gslpp::complex> MLH(3, 3, 0.0);
14163 
14164  MRH = sqrt(2.0) * 4.0 * M_PI * aleMz * (AmpZRH + AmpgaRH);
14165  MLH = - sqrt(2.0) * 4.0 * M_PI * aleMz * (AmpZLH + AmpgaLH + Ampnu1) + Ampnu2;
14166 
14167 // Total amplitude squared and differential cross section (in pb)
14168  gslpp::matrix<double> M2(3, 3, 0.0);
14169  double dxsdcos;
14170 
14171  dxsdcos = 0.0;
14172 
14173  for (int i=0; i<3; i++) {
14174  for (int j=0; j<3; j++) {
14175  M2.assign(i,j, (MRH(i,j)* (MRH(i,j).conjugate())
14176  + MLH(i,j)* (MLH(i,j).conjugate())).real() );
14177 
14178  dxsdcos = dxsdcos + M2(i,j);
14179  }
14180  }
14181 
14182 // Differential cross section in pb
14183  dxsdcos = (topb * beta / 32.0 / M_PI / s) * dxsdcos;
14184 
14185  return dxsdcos;
14186 }

◆ dxseeWWdcosBin()

double NPSMEFTd6::dxseeWWdcosBin ( const double  sqrt_s,
const double  cos1,
const double  cos2 
) const
virtual

The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.

Returns
\(\int_{\cos{\theta_1}}^{\cos{\theta_2}} d\sigma/d\cos{\theta}\)

< Gsl integral variable

< Gsl integral variable

< Gsl integral variable

Reimplemented from NPbase.

Definition at line 14188 of file NPSMEFTd6.cpp.

14189 {
14190  double xsWWbin;
14191  double errWW;
14193  gsl_function FR;
14195  FR = convertToGslFunction(boost::bind(&NPSMEFTd6::dxseeWWdcos,&(*this), sqrt_s, _1));
14196 
14197  gsl_integration_cquad(&FR, cos1, cos2, 1.e-5, 1.e-4, w_WW, &xsWWbin, &errWW, NULL);
14198 
14199 // Simple integration for testing
14200 // double cosx;
14201 
14202 // xsWWbin = 0.0;
14203 
14204 // for (int i=1; i<100; i++){
14205 // cosx = cos1 + i*(cos2-cos1)/100;
14206 // xsWWbin = xsWWbin + dxseeWWdcos(sqrt_s, cosx);
14207 // }
14208 
14209 // xsWWbin = xsWWbin + 0.5 * (dxseeWWdcos(sqrt_s, cos1) + dxseeWWdcos(sqrt_s, cos2));
14210 
14211 // xsWWbin = xsWWbin * (cos2-cos1)/100;
14212 
14213 // Compute the BR into e nu, mu nu for one W and into jets for the other
14214  double BRlv, BRjj;
14215 
14216  BRlv = GammaW(leptons[NEUTRINO_1], leptons[ELECTRON]) +
14219 
14220  BRjj = GammaW() - BRlv;
14221 
14222  BRlv = BRlv - GammaW(leptons[NEUTRINO_3], leptons[TAU]);
14223 
14224  BRlv =BRlv / GammaW();
14225 
14226  BRjj =BRjj / GammaW();
14227 
14228 
14229 
14230  return xsWWbin * BRlv * BRjj;
14231 }

◆ f_triangle()

gslpp::complex NPSMEFTd6::f_triangle ( const double  tau) const

Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.

Parameters
[in]

Definition at line 3551 of file NPSMEFTd6.cpp.

3552 {
3553  gslpp::complex tmp;
3554  if (tau >= 1.0) {
3555  tmp = asin(1.0 / sqrt(tau));
3556  return (tmp * tmp);
3557  } else {
3558  tmp = log((1.0 + sqrt(1.0 - tau)) / (1.0 - sqrt(1.0 - tau))) - M_PI * gslpp::complex::i();
3559  return (-0.25 * tmp * tmp);
3560  }
3561 }

◆ g_triangle()

gslpp::complex NPSMEFTd6::g_triangle ( const double  tau) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3563 of file NPSMEFTd6.cpp.

3564 {
3565  gslpp::complex tmp;
3566  if (tau >= 1.0) {
3567  tmp = sqrt(tau -1.0) * asin(1.0 / sqrt(tau));
3568  return tmp;
3569  } else {
3570  tmp = sqrt(1.0 - tau) * ( log((1.0 + sqrt(1.0 - tau)) / (1.0 - sqrt(1.0 - tau))) - M_PI * gslpp::complex::i() );
3571  return 0.5 * tmp;
3572  }
3573 }

◆ GammaHbbRatio()

double NPSMEFTd6::GammaHbbRatio ( ) const

The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to bb)\)/ \(\Gamma(H\to bb)_{\mathrm{SM}}\)

Definition at line 12648 of file NPSMEFTd6.cpp.

12649 {
12650  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12651  double width = 1.0;
12652 
12653  width += deltaGammaHbbRatio1();
12654 
12655  if (FlagQuadraticTerms) {
12656  //Add contributions that are quadratic in the effective coefficients
12657  width += deltaGammaHbbRatio2();
12658  }
12659 
12660  return width;
12661 }

◆ GammaHccRatio()

double NPSMEFTd6::GammaHccRatio ( ) const

The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to cc)\)/ \(\Gamma(H\to cc)_{\mathrm{SM}}\)

Definition at line 12582 of file NPSMEFTd6.cpp.

12583 {
12584  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12585  double width = 1.0;
12586 
12587  width += deltaGammaHccRatio1();
12588 
12589  if (FlagQuadraticTerms) {
12590  //Add contributions that are quadratic in the effective coefficients
12591  width += deltaGammaHccRatio2();
12592  }
12593 
12594  return width;
12595 
12596 }

◆ GammaHgagaRatio()

double NPSMEFTd6::GammaHgagaRatio ( ) const

The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \gamma\gamma)\)/ \(\Gamma(H\to \gamma\gamma)_{\mathrm{SM}}\)

Definition at line 12401 of file NPSMEFTd6.cpp.

12402 {
12403  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12404  double width = 1.0;
12405 
12406  width += deltaGammaHgagaRatio1();
12407 
12408  if (FlagQuadraticTerms) {
12409  //Add contributions that are quadratic in the effective coefficients
12410  width += deltaGammaHgagaRatio2();
12411  }
12412 
12413  return width;
12414 
12415 }

◆ GammaHggRatio()

double NPSMEFTd6::GammaHggRatio ( ) const

The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to gg)\)/ \(\Gamma(H\to gg)_{\mathrm{SM}}\)

Definition at line 10972 of file NPSMEFTd6.cpp.

10973 {
10974  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
10975  double width = 1.0;
10976 
10977  width += deltaGammaHggRatio1();
10978 
10979  if (FlagQuadraticTerms) {
10980  //Add contributions that are quadratic in the effective coefficients
10981  width += deltaGammaHggRatio2();
10982  }
10983 
10984  return width;
10985 
10986 }

◆ GammaHmumuRatio()

double NPSMEFTd6::GammaHmumuRatio ( ) const

The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \mu\mu)\)/ \(\Gamma(H\to \mu\mu)_{\mathrm{SM}}\)

Definition at line 12477 of file NPSMEFTd6.cpp.

12478 {
12479  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12480  double width = 1.0;
12481 
12482  width += deltaGammaHmumuRatio1();
12483 
12484  if (FlagQuadraticTerms) {
12485  //Add contributions that are quadratic in the effective coefficients
12486  width += deltaGammaHmumuRatio2();
12487  }
12488 
12489  return width;
12490 
12491 }

◆ GammaHtautauRatio()

double NPSMEFTd6::GammaHtautauRatio ( ) const

The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to \tau\tau)\)/ \(\Gamma(H\to \tau\tau)_{\mathrm{SM}}\)

Definition at line 12529 of file NPSMEFTd6.cpp.

12530 {
12531  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12532  double width = 1.0;
12533 
12534  width += deltaGammaHtautauRatio1();
12535 
12536  if (FlagQuadraticTerms) {
12537  //Add contributions that are quadratic in the effective coefficients
12538  width += deltaGammaHtautauRatio2();
12539  }
12540 
12541  return width;
12542 
12543 }

◆ GammaHWffRatio()

double NPSMEFTd6::GammaHWffRatio ( ) const

The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to W f f)\)/ \(\Gamma(H\to W f f)_{\mathrm{SM}}\)

Definition at line 11314 of file NPSMEFTd6.cpp.

11315 {
11316  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11317  double width = 1.0;
11318 
11319  width += deltaGammaHWffRatio1();
11320 
11321  if (FlagQuadraticTerms) {
11322  //Add contributions that are quadratic in the effective coefficients
11323  width += deltaGammaHWffRatio2();
11324  }
11325 
11326  return width;
11327 
11328 }

◆ GammaHWjjRatio()

double NPSMEFTd6::GammaHWjjRatio ( ) const

The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to W j j)\)/ \(\Gamma(H\to W j j)_{\mathrm{SM}}\)

Definition at line 11198 of file NPSMEFTd6.cpp.

11199 {
11200  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11201  double width = 1.0;
11202 
11203  width += deltaGammaHWjjRatio1();
11204 
11205  if (FlagQuadraticTerms) {
11206  //Add contributions that are quadratic in the effective coefficients
11207  width += deltaGammaHWjjRatio2();
11208  }
11209 
11210  return width;
11211 
11212 }

◆ GammaHWlvRatio()

double NPSMEFTd6::GammaHWlvRatio ( ) const

The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Wl\nu)\)/ \(\Gamma(H\to Wl\nu)_{\mathrm{SM}}\)

Definition at line 11081 of file NPSMEFTd6.cpp.

11082 {
11083  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11084  double width = 1.0;
11085 
11086  width += deltaGammaHWlvRatio1();
11087 
11088  if (FlagQuadraticTerms) {
11089  //Add contributions that are quadratic in the effective coefficients
11090  width += deltaGammaHWlvRatio2();
11091  }
11092 
11093  return width;
11094 
11095 }

◆ GammaHWW2l2vRatio()

double NPSMEFTd6::GammaHWW2l2vRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to l\nu l\nu)\)/ \(\Gamma(H\to WW^*\to l\nu l\nu)_{\mathrm{SM}}\)

Definition at line 11137 of file NPSMEFTd6.cpp.

11138 {
11139  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11140  double width = 1.0;
11141 
11142  width += deltaGammaHWW2l2vRatio1();
11143 
11144  if (FlagQuadraticTerms) {
11145  //Add contributions that are quadratic in the effective coefficients
11146  width += deltaGammaHWW2l2vRatio2();
11147  }
11148 
11149  return width;
11150 
11151 }

◆ GammaHWW4fRatio()

double NPSMEFTd6::GammaHWW4fRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to 4f)\)/ \(\Gamma(H\to WW^*\to 4f)_{\mathrm{SM}}\)

Definition at line 11371 of file NPSMEFTd6.cpp.

11372 {
11373  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11374  double width = 1.0;
11375 
11376  width += deltaGammaHWW4fRatio1();
11377 
11378  if (FlagQuadraticTerms) {
11379  //Add contributions that are quadratic in the effective coefficients
11380  width += deltaGammaHWW4fRatio2();
11381  }
11382 
11383  return width;
11384 
11385 }

◆ GammaHWW4jRatio()

double NPSMEFTd6::GammaHWW4jRatio ( ) const

The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW^*\to 4j)\)/ \(\Gamma(H\to WW^*\to 4j)_{\mathrm{SM}}\)

Definition at line 11254 of file NPSMEFTd6.cpp.

11255 {
11256  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11257  double width = 1.0;
11258 
11259  width += deltaGammaHWW4jRatio1();
11260 
11261  if (FlagQuadraticTerms) {
11262  //Add contributions that are quadratic in the effective coefficients
11263  width += deltaGammaHWW4jRatio2();
11264  }
11265 
11266  return width;
11267 
11268 }

◆ GammaHWWRatio()

double NPSMEFTd6::GammaHWWRatio ( ) const

The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to WW)\)/ \(\Gamma(H\to WW)_{\mathrm{SM}}\)

Definition at line 11033 of file NPSMEFTd6.cpp.

11034 {
11035  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11036  double width = 1.0;
11037 
11038  width += deltaGammaHWWRatio1();
11039 
11040  if (FlagQuadraticTerms) {
11041  //Add contributions that are quadratic in the effective coefficients
11042  width += deltaGammaHWWRatio2();
11043  }
11044 
11045  return width;
11046 
11047 }

◆ GammaHZddRatio()

double NPSMEFTd6::GammaHZddRatio ( ) const

The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zd d)\)/ \(\Gamma(H\to Zd d)_{\mathrm{SM}}\)

Definition at line 12108 of file NPSMEFTd6.cpp.

12109 {
12110  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12111  double width = 1.0;
12112 
12113  width += deltaGammaHZddRatio1();
12114 
12115  if (FlagQuadraticTerms) {
12116  //Add contributions that are quadratic in the effective coefficients
12117  width += deltaGammaHZddRatio2();
12118  }
12119 
12120  return width;
12121 
12122 }

◆ GammaHZeeRatio()

double NPSMEFTd6::GammaHZeeRatio ( ) const

The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zee)\)/ \(\Gamma(H\to Zee)_{\mathrm{SM}}\)

Definition at line 11548 of file NPSMEFTd6.cpp.

11549 {
11550  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11551  double width = 1.0;
11552 
11553  width += deltaGammaHZeeRatio1();
11554 
11555  if (FlagQuadraticTerms) {
11556  //Add contributions that are quadratic in the effective coefficients
11557  width += deltaGammaHZeeRatio2();
11558  }
11559 
11560  return width;
11561 
11562 }

◆ GammaHZffRatio()

double NPSMEFTd6::GammaHZffRatio ( ) const

The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zff)\)/ \(\Gamma(H\to Zff)_{\mathrm{SM}}\)

Definition at line 12167 of file NPSMEFTd6.cpp.

12168 {
12169  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12170  double width = 1.0;
12171 
12172  width += deltaGammaHZffRatio1();
12173 
12174  if (FlagQuadraticTerms) {
12175  //Add contributions that are quadratic in the effective coefficients
12176  width += deltaGammaHZffRatio2();
12177  }
12178 
12179  return width;
12180 
12181 }

◆ GammaHZgaRatio()

double NPSMEFTd6::GammaHZgaRatio ( ) const

The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\gamma)\)/ \(\Gamma(H\to Z\gamma)_{\mathrm{SM}}\)

Definition at line 12316 of file NPSMEFTd6.cpp.

12317 {
12318  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12319  double width = 1.0;
12320 
12321  width += deltaGammaHZgaRatio1();
12322 
12323  if (FlagQuadraticTerms) {
12324  //Add contributions that are quadratic in the effective coefficients
12325  width += deltaGammaHZgaRatio2();
12326  }
12327 
12328  return width;
12329 
12330 }

◆ GammaHZllRatio()

double NPSMEFTd6::GammaHZllRatio ( ) const

The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zll)\)/ \(\Gamma(H\to Zll)_{\mathrm{SM}}\)

Definition at line 11489 of file NPSMEFTd6.cpp.

11490 {
11491  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11492  double width = 1.0;
11493 
11494  width += deltaGammaHZllRatio1();
11495 
11496  if (FlagQuadraticTerms) {
11497  //Add contributions that are quadratic in the effective coefficients
11498  width += deltaGammaHZllRatio2();
11499  }
11500 
11501  return width;
11502 
11503 }

◆ GammaHZmumuRatio()

double NPSMEFTd6::GammaHZmumuRatio ( ) const

The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\mu\mu)\)/ \(\Gamma(H\to Z\mu\mu)_{\mathrm{SM}}\)

Definition at line 11609 of file NPSMEFTd6.cpp.

11610 {
11611  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11612  double width = 1.0;
11613 
11614  width += deltaGammaHZmumuRatio1();
11615 
11616  if (FlagQuadraticTerms) {
11617  //Add contributions that are quadratic in the effective coefficients
11618  width += deltaGammaHZmumuRatio2();
11619  }
11620 
11621  return width;
11622 
11623 }

◆ GammaHZuuRatio()

double NPSMEFTd6::GammaHZuuRatio ( ) const

The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Zu u)\)/ \(\Gamma(H\to Zu u)_{\mathrm{SM}}\)

Definition at line 12049 of file NPSMEFTd6.cpp.

12050 {
12051  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12052  double width = 1.0;
12053 
12054  width += deltaGammaHZuuRatio1();
12055 
12056  if (FlagQuadraticTerms) {
12057  //Add contributions that are quadratic in the effective coefficients
12058  width += deltaGammaHZuuRatio2();
12059  }
12060 
12061  return width;
12062 
12063 }

◆ GammaHZvvRatio()

double NPSMEFTd6::GammaHZvvRatio ( ) const

The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to Z\nu\nu)\)/ \(\Gamma(H\to Z\nu\nu)_{\mathrm{SM}}\)

Definition at line 11928 of file NPSMEFTd6.cpp.

11929 {
11930  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11931  double width = 1.0;
11932 
11933  width += deltaGammaHZvvRatio1();
11934 
11935  if (FlagQuadraticTerms) {
11936  //Add contributions that are quadratic in the effective coefficients
11937  width += deltaGammaHZvvRatio2();
11938  }
11939 
11940  return width;
11941 
11942 }

◆ GammaHZZ2e2muRatio()

double NPSMEFTd6::GammaHZZ2e2muRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 2e2\mu)\)/ \(\Gamma(H\to ZZ* \to 2e2\mu)_{\mathrm{SM}}\)

Definition at line 11803 of file NPSMEFTd6.cpp.

11804 {
11805  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11806  double width = 1.0;
11807 
11808  width += deltaGammaHZZ2e2muRatio1();
11809 
11810  if (FlagQuadraticTerms) {
11811  //Add contributions that are quadratic in the effective coefficients
11812  width += deltaGammaHZZ2e2muRatio2();
11813  }
11814 
11815  return width;
11816 
11817 }

◆ GammaHZZ4dRatio()

double NPSMEFTd6::GammaHZZ4dRatio ( ) const
inline

The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4 d)\)/ \(\Gamma(H\to ZZ* \to 4 d)_{\mathrm{SM}}\)

Definition at line 2315 of file NPSMEFTd6.h.

2316  {
2317  return 1.0;
2318  };

◆ GammaHZZ4eRatio()

double NPSMEFTd6::GammaHZZ4eRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4e)\)/ \(\Gamma(H\to ZZ* \to 4e)_{\mathrm{SM}}\)

Definition at line 11740 of file NPSMEFTd6.cpp.

11741 {
11742  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11743  double width = 1.0;
11744 
11745  width += deltaGammaHZZ4eRatio1();
11746 
11747  if (FlagQuadraticTerms) {
11748  //Add contributions that are quadratic in the effective coefficients
11749  width += deltaGammaHZZ4eRatio2();
11750  }
11751 
11752  return width;
11753 
11754 }

◆ GammaHZZ4fRatio()

double NPSMEFTd6::GammaHZZ4fRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4f)\)/ \(\Gamma(H\to ZZ* \to 4f)_{\mathrm{SM}}\)

Definition at line 12230 of file NPSMEFTd6.cpp.

12231 {
12232  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
12233  double width = 1.0;
12234 
12235  width += deltaGammaHZZ4fRatio1();
12236 
12237  if (FlagQuadraticTerms) {
12238  //Add contributions that are quadratic in the effective coefficients
12239  width += deltaGammaHZZ4fRatio2();
12240  }
12241 
12242  return width;
12243 
12244 }

◆ GammaHZZ4lRatio()

double NPSMEFTd6::GammaHZZ4lRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4l)\)/ \(\Gamma(H\to ZZ* \to 4l)_{\mathrm{SM}}\)

Definition at line 11670 of file NPSMEFTd6.cpp.

11671 {
11672  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11673  double width = 1.0;
11674 
11675  width += deltaGammaHZZ4lRatio1();
11676 
11677  if (FlagQuadraticTerms) {
11678  //Add contributions that are quadratic in the effective coefficients
11679  width += deltaGammaHZZ4lRatio2();
11680  }
11681 
11682  return width;
11683 
11684 }

◆ GammaHZZ4muRatio()

double NPSMEFTd6::GammaHZZ4muRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4\mu)\)/ \(\Gamma(H\to ZZ* \to 4\mu)_{\mathrm{SM}}\)

Definition at line 11865 of file NPSMEFTd6.cpp.

11866 {
11867  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11868  double width = 1.0;
11869 
11870  width += deltaGammaHZZ4muRatio1();
11871 
11872  if (FlagQuadraticTerms) {
11873  //Add contributions that are quadratic in the effective coefficients
11874  width += deltaGammaHZZ4muRatio2();
11875  }
11876 
11877  return width;
11878 
11879 }

◆ GammaHZZ4uRatio()

double NPSMEFTd6::GammaHZZ4uRatio ( ) const
inline

The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4u)\)/ \(\Gamma(H\to ZZ* \to 4u)_{\mathrm{SM}}\)

Definition at line 2300 of file NPSMEFTd6.h.

2301  {
2302  return 1.0;
2303  };

◆ GammaHZZ4vRatio()

double NPSMEFTd6::GammaHZZ4vRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ* \to 4\nu)\)/ \(\Gamma(H\to ZZ* \to 4\nu)_{\mathrm{SM}}\)

Definition at line 11986 of file NPSMEFTd6.cpp.

11987 {
11988  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11989  double width = 1.0;
11990 
11991  width += deltaGammaHZZ4vRatio1();
11992 
11993  if (FlagQuadraticTerms) {
11994  //Add contributions that are quadratic in the effective coefficients
11995  width += deltaGammaHZZ4vRatio2();
11996  }
11997 
11998  return width;
11999 
12000 }

◆ GammaHZZRatio()

double NPSMEFTd6::GammaHZZRatio ( ) const

The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.

Returns
\(\Gamma(H\to ZZ)\)/ \(\Gamma(H\to ZZ)_{\mathrm{SM}}\)

Definition at line 11441 of file NPSMEFTd6.cpp.

11442 {
11443  // SM (1). Intrinsic + parametric theory relative errors (free pars) included in deltaGammaHXXRatio1
11444  double width = 1.0;
11445 
11446  width += deltaGammaHZZRatio1();
11447 
11448  if (FlagQuadraticTerms) {
11449  //Add contributions that are quadratic in the effective coefficients
11450  width += deltaGammaHZZRatio2();
11451  }
11452 
11453  return width;
11454 
11455 }

◆ GammaW() [1/2]

double NPSMEFTd6::GammaW ( ) const
virtual

The total width of the \(W\) boson, \(\Gamma_W\).

Returns
\(\Gamma_W\) in GeV

Reimplemented from NPbase.

Definition at line 3137 of file NPSMEFTd6.cpp.

3138 {
3139  return ( trueSM.GammaW() + deltaGamma_W() );
3140 }

◆ GammaW() [2/2]

double NPSMEFTd6::GammaW ( const Particle  fi,
const Particle  fj 
) const
virtual

A partial decay width of the \(W\) boson decay into a SM fermion pair.

Parameters
[in]fia lepton or quark
[in]fja lepton or quark
Returns
\(\Gamma^W_{ij}\)

Reimplemented from NPbase.

Definition at line 3119 of file NPSMEFTd6.cpp.

3120 {
3121  return ( trueSM.GammaW(fi, fj) + deltaGamma_Wff(fi, fj) );
3122 }

◆ getCed_1123()

double NPSMEFTd6::getCed_1123 ( ) const
inline

Return NP coeff Ced_1123.

Returns
\( Ced_1123 \)

Definition at line 1044 of file NPSMEFTd6.h.

1044  {
1045  return Ced_1123;
1046  }

◆ getCed_2223()

double NPSMEFTd6::getCed_2223 ( ) const
inline

Return NP coeff Ced_2223.

Returns
\( Ced_2223 \)

Definition at line 1052 of file NPSMEFTd6.h.

1052  {
1053  return Ced_2223;
1054  }

◆ getCeu_1133()

double NPSMEFTd6::getCeu_1133 ( ) const
inline

Return NP coeff Ceu_1133.

Returns
\( Ceu_1133 \)

Definition at line 1108 of file NPSMEFTd6.h.

1108  {
1109  return Ceu_1133;
1110  }

◆ getCeu_2233()

double NPSMEFTd6::getCeu_2233 ( ) const
inline

Return NP coeff Ceu_2233.

Returns
\( Ceu_2233 \)

Definition at line 1116 of file NPSMEFTd6.h.

1116  {
1117  return Ceu_2233;
1118  }

◆ getCHe_11()

double NPSMEFTd6::getCHe_11 ( ) const
inline

Return NP coeff CHe_11.

Returns
\( CHe_11 \)

Definition at line 1092 of file NPSMEFTd6.h.

1092  {
1093  return CHe_11;
1094  }

◆ getCHe_22()

double NPSMEFTd6::getCHe_22 ( ) const
inline

Return NP coeff CHe_22.

Returns
\( CHe_22 \)

Definition at line 1100 of file NPSMEFTd6.h.

1100  {
1101  return CHe_22;
1102  }

◆ getCHL1_11()

double NPSMEFTd6::getCHL1_11 ( ) const
inline

Return NP coeff CHL1_11.

Returns
\( CHL1_11 \)

Definition at line 1060 of file NPSMEFTd6.h.

1060  {
1061  return CHL1_11;
1062  }

◆ getCHL1_22()

double NPSMEFTd6::getCHL1_22 ( ) const
inline

Return NP coeff CHL1_22.

Returns
\( CHL1_22 \)

Definition at line 1068 of file NPSMEFTd6.h.

1068  {
1069  return CHL1_22;
1070  }

◆ getCHL3_11()

double NPSMEFTd6::getCHL3_11 ( ) const
inline

Return NP coeff CHL3_11.

Returns
\( CHL3_11 \)

Definition at line 1076 of file NPSMEFTd6.h.

1076  {
1077  return CHL3_11;
1078  }

◆ getCHL3_22()

double NPSMEFTd6::getCHL3_22 ( ) const
inline

Return NP coeff CHL3_22.

Returns
\( CHL3_22 \)

Definition at line 1084 of file NPSMEFTd6.h.

1084  {
1085  return CHL3_22;
1086  }

◆ getCLd_1123()

double NPSMEFTd6::getCLd_1123 ( ) const
inline

Return NP coeff CLd_1123.

Returns
\( CLd_1123 \)

Definition at line 1028 of file NPSMEFTd6.h.

1028  {
1029  return CLd_1123;
1030  }

◆ getCLd_2223()

double NPSMEFTd6::getCLd_2223 ( ) const
inline

Return NP coeff CLd_2223.

Returns
\( CLd_2223 \)

Definition at line 1036 of file NPSMEFTd6.h.

1036  {
1037  return CLd_2223;
1038  }

◆ getCLedQ_11()

double NPSMEFTd6::getCLedQ_11 ( ) const
inline

Return NP coeff CLedq_11.

Returns
\( CLedq_11 \)

Definition at line 1140 of file NPSMEFTd6.h.

1140  {
1141  return CLedQ_11;
1142  }

◆ getCLedQ_22()

double NPSMEFTd6::getCLedQ_22 ( ) const
inline

Return NP coeff CLedq_22.

Returns
\( CLedq_22 \)

Definition at line 1148 of file NPSMEFTd6.h.

1148  {
1149  return CLedQ_22;
1150  }

◆ getCLQ1_1123()

double NPSMEFTd6::getCLQ1_1123 ( ) const
inline

Return NP coeff CLQ1_1123.

Returns
\( CLQ1_1123 \)

Definition at line 996 of file NPSMEFTd6.h.

996  {
997  return CLQ1_1123;
998  }

◆ getCLQ1_2223()

double NPSMEFTd6::getCLQ1_2223 ( ) const
inline

Return NP coeff CLQ1_2223.

Returns
\( CLQ1_2223 \)

Definition at line 1004 of file NPSMEFTd6.h.

1004  {
1005  return CLQ1_2223;
1006  }

◆ getCLQ3_1123()

double NPSMEFTd6::getCLQ3_1123 ( ) const
inline

Return NP coeff CLQ3_1123.

Returns
\( CLQ3_1123 \)

Definition at line 1012 of file NPSMEFTd6.h.

1012  {
1013  return CLQ3_1123;
1014  }

◆ getCLQ3_2223()

double NPSMEFTd6::getCLQ3_2223 ( ) const
inline

Return NP coeff CLQ3_2223.

Returns
\( CLQ3_2223 \)

Definition at line 1020 of file NPSMEFTd6.h.

1020  {
1021  return CLQ3_2223;
1022  }

◆ getCLu_1133()

double NPSMEFTd6::getCLu_1133 ( ) const
inline

Return NP coeff CLu_1133.

Returns
\( CLu_1133 \)

Definition at line 1124 of file NPSMEFTd6.h.

1124  {
1125  return CLu_1133;
1126  }

◆ getCLu_2233()

double NPSMEFTd6::getCLu_2233 ( ) const
inline

Return NP coeff CLu_2233.

Returns
\( CLu_2233 \)

Definition at line 1132 of file NPSMEFTd6.h.

1132  {
1133  return CLu_2233;
1134  }

◆ getCpLedQ_11()

double NPSMEFTd6::getCpLedQ_11 ( ) const
inline

Return NP coeff CpLedq_11.

Returns
\( CpLedq_11 \)

Definition at line 1156 of file NPSMEFTd6.h.

1156  {
1157  return CpLedQ_11;
1158  }

◆ getCpLedQ_22()

double NPSMEFTd6::getCpLedQ_22 ( ) const
inline

Return NP coeff CpLedq_22.

Returns
\( CpLedq \)

Definition at line 1164 of file NPSMEFTd6.h.

1164  {
1165  return CpLedQ_22;
1166  }

◆ getCQe_2311()

double NPSMEFTd6::getCQe_2311 ( ) const
inline

Return NP coeff CQe_2322.

Returns
\( CQe_2322 \)

Definition at line 980 of file NPSMEFTd6.h.

980  {
981  return CQe_2311;
982  }

◆ getCQe_2322()

double NPSMEFTd6::getCQe_2322 ( ) const
inline

Return NP coeff CQe_2322.

Returns
\( CQe_2311 \)

Definition at line 988 of file NPSMEFTd6.h.

988  {
989  return CQe_2322;
990  }

◆ getLambda_NP()

double NPSMEFTd6::getLambda_NP ( ) const
inline

Return Lambda_NP.

Returns
\( Lambda_NP \)

Definition at line 972 of file NPSMEFTd6.h.

972  {
973  return Lambda_NP;
974  }

◆ getMatching()

virtual NPSMEFTd6Matching& NPSMEFTd6::getMatching ( ) const
inlinevirtual

A method to get the Matching object for this model.

Returns
The matching object for this model

Reimplemented from StandardModel.

Definition at line 961 of file NPSMEFTd6.h.

962  {
963  return NPSMEFTd6M.getObj();
964  }

◆ I_triangle_1()

gslpp::complex NPSMEFTd6::I_triangle_1 ( const double  tau,
const double  lambda 
) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3575 of file NPSMEFTd6.cpp.

3576 {
3577  gslpp::complex tmp;
3578 
3579  tmp = ( tau*lambda * (f_triangle(tau)- f_triangle(lambda)) + 2.0 * tau * (g_triangle(tau)- g_triangle(lambda)) ) / (tau-lambda);
3580 
3581  tmp = tau*lambda * ( 1.0 + tmp ) / (2.0*(tau-lambda));
3582 
3583  return tmp;
3584 }

◆ I_triangle_2()

gslpp::complex NPSMEFTd6::I_triangle_2 ( const double  tau,
const double  lambda 
) const

Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.

Parameters
[in]

Definition at line 3586 of file NPSMEFTd6.cpp.

3587 {
3588  gslpp::complex tmp;
3589 
3590  tmp = - 0.5 * tau*lambda * (f_triangle(tau)- f_triangle(lambda)) / (tau-lambda);
3591 
3592  return tmp;
3593 }

◆ kappaAeff()

double NPSMEFTd6::kappaAeff ( ) const
virtual

The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).

Returns
\(\kappa_{A,eff}\)

Reimplemented from NPbase.

Definition at line 15455 of file NPSMEFTd6.cpp.

15456 {
15457  return sqrt(GammaHgagaRatio());
15458 }

◆ kappabeff()

double NPSMEFTd6::kappabeff ( ) const
virtual

The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).

Returns
\(\kappa_{b,eff}\)

Reimplemented from NPbase.

Definition at line 15435 of file NPSMEFTd6.cpp.

15436 {
15437  return sqrt(GammaHbbRatio());
15438 }

◆ kappaceff()

double NPSMEFTd6::kappaceff ( ) const
virtual

The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).

Returns
\(\kappa_{c,eff}\)

Reimplemented from NPbase.

Definition at line 15430 of file NPSMEFTd6.cpp.

15431 {
15432  return sqrt(GammaHccRatio());
15433 }

◆ kappaGeff()

double NPSMEFTd6::kappaGeff ( ) const
virtual

The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).

Returns
\(\kappa_{G,eff}\)

Reimplemented from NPbase.

Definition at line 15440 of file NPSMEFTd6.cpp.

15441 {
15442  return sqrt(GammaHggRatio());
15443 }

◆ kappamueff()

double NPSMEFTd6::kappamueff ( ) const
virtual

The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).

Returns
\(\kappa_{\mu,eff}\)

Reimplemented from NPbase.

Definition at line 15420 of file NPSMEFTd6.cpp.

15421 {
15422  return sqrt(GammaHmumuRatio());
15423 }

◆ kappataueff()

double NPSMEFTd6::kappataueff ( ) const
virtual

The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).

Returns
\(\kappa_{\tau,eff}\)

Reimplemented from NPbase.

Definition at line 15425 of file NPSMEFTd6.cpp.

15426 {
15427  return sqrt(GammaHtautauRatio());
15428 }

◆ kappaWeff()

double NPSMEFTd6::kappaWeff ( ) const
virtual

The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).

Returns
\(\kappa_{W,eff}\)

Reimplemented from NPbase.

Definition at line 15450 of file NPSMEFTd6.cpp.

15451 {
15452  return sqrt(GammaHWWRatio());
15453 }

◆ kappaZAeff()

double NPSMEFTd6::kappaZAeff ( ) const
virtual

The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).

Returns
\(\kappa_{ZA,eff}\)

Reimplemented from NPbase.

Definition at line 15460 of file NPSMEFTd6.cpp.

15461 {
15462  return sqrt(GammaHZgaRatio());
15463 }

◆ kappaZeff()

double NPSMEFTd6::kappaZeff ( ) const
virtual

The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).

Returns
\(\kappa_{Z,eff}\)

Reimplemented from NPbase.

Definition at line 15445 of file NPSMEFTd6.cpp.

15446 {
15447  return sqrt(GammaHZZRatio());
15448 }

◆ lambdaZNP()

double NPSMEFTd6::lambdaZNP ( ) const
virtual

The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).

Returns
\(\lambda_{Z}\)

Reimplemented from NPbase.

Definition at line 13850 of file NPSMEFTd6.cpp.

13851 {
13852  double NPdirect;
13853 
13854  /* Translate from LHCHXWG-INT-2015-001: Checked with own calculations */
13855  NPdirect = - (3.0 / 2.0) * (sqrt( 4.0 * M_PI * aleMz ) / sW_tree) * CiW * v2_over_LambdaNP2;
13856 
13857  return NPdirect + lambZ ;
13858 }

◆ lambz_HB()

double NPSMEFTd6::lambz_HB ( ) const
virtual

The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).

Returns
\(\lambda_{z}\)

Reimplemented from NPbase.

Definition at line 15608 of file NPSMEFTd6.cpp.

15609 {
15610  double ciHB;
15611 
15612  ciHB = -(3.0/2.0)*(eeMz/sW_tree)*CiW*v2_over_LambdaNP2;
15613 
15614  return ciHB;
15615 }

◆ mueeHvv()

double NPSMEFTd6::mueeHvv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{e^+e^- \to H\nu\bar{\nu}}\)

Reimplemented from NPbase.

Definition at line 4320 of file NPSMEFTd6.cpp.

4321 {
4322  double mu = 1.0;
4323 
4324  double C1 = 0.0;
4325 
4326 // For the Higgs trilinear dependence assume the WBF mechanism dominates
4327 
4328  if (sqrt_s == 0.240) {
4329 
4330  C1 = 0.0064;
4331 
4332  mu +=
4333  +121539. * CiHbox / LambdaNP2
4334  +328845. * CiHL1_11 / LambdaNP2
4335  -37798.9 * CiHe_11 / LambdaNP2
4336  +279733. * CiHL3_11 / LambdaNP2
4337  -196039. * CiHD / LambdaNP2
4338  -70718.5 * CiHB / LambdaNP2
4339  +29671.9 * CiHW / LambdaNP2
4340  -401378. * CiHWB / LambdaNP2
4341  -23969.3 * CiDHB / LambdaNP2
4342  -1814.47 * CiDHW / LambdaNP2
4343  -4.698 * DeltaGF()
4344  -5.463 * deltaMwd6()
4345  ;
4346 
4347  // Add modifications due to small variations of the SM parameters
4348  mu += cHSM * (
4349  +4.842 * deltaMz()
4350  -2.535 * deltaMh()
4351  -0.528 * deltaaMZ()
4352  +3.46 * deltaGmu() );
4353 
4354  if (FlagQuadraticTerms) {
4355  //Add contributions that are quadratic in the effective coefficients
4356  mu += 0.0;
4357  }
4358 
4359  } else if (sqrt_s == 0.250) {
4360 
4361  C1 = 0.0064;
4362 
4363  mu +=
4364  +120627. * CiHbox / LambdaNP2
4365  +256825. * CiHL1_11 / LambdaNP2
4366  -38677.5 * CiHe_11 / LambdaNP2
4367  +175735. * CiHL3_11 / LambdaNP2
4368  -201059. * CiHD / LambdaNP2
4369  -57405. * CiHB / LambdaNP2
4370  -9860.82 * CiHW / LambdaNP2
4371  -403474. * CiHWB / LambdaNP2
4372  -20447.1 * CiDHB / LambdaNP2
4373  -9672.74 * CiDHW / LambdaNP2
4374  -4.656 * DeltaGF()
4375  -5.633 * deltaMwd6()
4376  ;
4377 
4378  // Add modifications due to small variations of the SM parameters
4379  mu += cHSM * (
4380  +4.194 * deltaMz()
4381  -2.783 * deltaMh()
4382  -0.477 * deltaaMZ()
4383  +3.414 * deltaGmu() );
4384 
4385  if (FlagQuadraticTerms) {
4386  //Add contributions that are quadratic in the effective coefficients
4387  mu += 0.0;
4388  }
4389 
4390  } else if (sqrt_s == 0.350) {
4391 
4392  C1 = 0.0062;
4393 
4394  mu +=
4395  +120666. * CiHbox / LambdaNP2
4396  -19184.6 * CiHL1_11 / LambdaNP2
4397  -27432.1 * CiHe_11 / LambdaNP2
4398  -238244. * CiHL3_11 / LambdaNP2
4399  -204898. * CiHD / LambdaNP2
4400  +11833.5 * CiHB / LambdaNP2
4401  -94273.3 * CiHW / LambdaNP2
4402  -377703. * CiHWB / LambdaNP2
4403  +1111.63 * CiDHB / LambdaNP2
4404  -31735.2 * CiDHW / LambdaNP2
4405  -4.669 * DeltaGF()
4406  -5.329 * deltaMwd6()
4407  ;
4408 
4409  // Add modifications due to small variations of the SM parameters
4410  mu += cHSM * (
4411  +3.738 * deltaMz()
4412  -1.994 * deltaMh()
4413  -0.537 * deltaaMZ()
4414  +3.484 * deltaGmu() );
4415 
4416  if (FlagQuadraticTerms) {
4417  //Add contributions that are quadratic in the effective coefficients
4418  mu += 0.0;
4419  }
4420 
4421  } else if (sqrt_s == 0.365) {
4422 
4423  C1 = 0.0062; // Use the same as 350 GeV
4424 
4425  mu +=
4426  +120864. * CiHbox / LambdaNP2
4427  -24430. * CiHL1_11 / LambdaNP2
4428  -24398.7 * CiHe_11 / LambdaNP2
4429  -253414. * CiHL3_11 / LambdaNP2
4430  -204817. * CiHD / LambdaNP2
4431  +12826.5 * CiHB / LambdaNP2
4432  -93455. * CiHW / LambdaNP2
4433  -377489. * CiHWB / LambdaNP2
4434  +1693.48 * CiDHB / LambdaNP2
4435  -32834.7 * CiDHW / LambdaNP2
4436  -4.68 * DeltaGF()
4437  -5.265 * deltaMwd6()
4438  ;
4439 
4440  // Add modifications due to small variations of the SM parameters
4441  mu += cHSM * (
4442  +3.834 * deltaMz()
4443  -1.867 * deltaMh()
4444  -0.556 * deltaaMZ()
4445  +3.512 * deltaGmu() );
4446 
4447  if (FlagQuadraticTerms) {
4448  //Add contributions that are quadratic in the effective coefficients
4449  mu += 0.0;
4450  }
4451 
4452  } else if (sqrt_s == 0.380) {
4453 
4454  C1 = 0.0062; // Use the same as 350 GeV
4455 
4456  mu +=
4457  +120775. * CiHbox / LambdaNP2
4458  -27548.7 * CiHL1_11 / LambdaNP2
4459  -22022.3 * CiHe_11 / LambdaNP2
4460  -266603. * CiHL3_11 / LambdaNP2
4461  -204782. * CiHD / LambdaNP2
4462  +13052.3 * CiHB / LambdaNP2
4463  -92560.2 * CiHW / LambdaNP2
4464  -377461. * CiHWB / LambdaNP2
4465  +1916.19 * CiDHB / LambdaNP2
4466  -33824.9 * CiDHW / LambdaNP2
4467  -4.684 * DeltaGF()
4468  -5.221 * deltaMwd6()
4469  ;
4470 
4471  // Add modifications due to small variations of the SM parameters
4472  mu += cHSM * (
4473  +3.931 * deltaMz()
4474  -1.75 * deltaMh()
4475  -0.574 * deltaaMZ()
4476  +3.532 * deltaGmu() );
4477 
4478  if (FlagQuadraticTerms) {
4479  //Add contributions that are quadratic in the effective coefficients
4480  mu += 0.0;
4481  }
4482 
4483  } else if (sqrt_s == 0.500) {
4484 
4485  C1 = 0.0061;
4486 
4487  mu +=
4488  +120683. * CiHbox / LambdaNP2
4489  -26906.2 * CiHL1_11 / LambdaNP2
4490  -11055.8 * CiHe_11 / LambdaNP2
4491  -326940. * CiHL3_11 / LambdaNP2
4492  -204335. * CiHD / LambdaNP2
4493  +10505.8 * CiHB / LambdaNP2
4494  -82453.1 * CiHW / LambdaNP2
4495  -378407. * CiHWB / LambdaNP2
4496  +1889.64 * CiDHB / LambdaNP2
4497  -41332.3 * CiDHW / LambdaNP2
4498  -4.705 * DeltaGF()
4499  -4.943 * deltaMwd6()
4500  ;
4501 
4502  // Add modifications due to small variations of the SM parameters
4503  mu += cHSM * (
4504  +4.412 * deltaMz()
4505  -1.191 * deltaMh()
4506  -0.659 * deltaaMZ()
4507  +3.633 * deltaGmu() );
4508 
4509  if (FlagQuadraticTerms) {
4510  //Add contributions that are quadratic in the effective coefficients
4511  mu += 0.0;
4512  }
4513 
4514  } else if (sqrt_s == 1.0) {
4515 
4516  C1 = 0.0059;
4517 
4518  mu +=
4519  +120462. * CiHbox / LambdaNP2
4520  -9025.99 * CiHL1_11 / LambdaNP2
4521  -3124.38 * CiHe_11 / LambdaNP2
4522  -454282. * CiHL3_11 / LambdaNP2
4523  -204077. * CiHD / LambdaNP2
4524  +3421.94 * CiHB / LambdaNP2
4525  -61892.5 * CiHW / LambdaNP2
4526  -379786. * CiHWB / LambdaNP2
4527  +396.747 * CiDHB / LambdaNP2
4528  -63826.6 * CiDHW / LambdaNP2
4529  -4.711 * DeltaGF()
4530  -4.587 * deltaMwd6()
4531  ;
4532 
4533  // Add modifications due to small variations of the SM parameters
4534  mu += cHSM * (
4535  +4.969 * deltaMz()
4536  -0.583 * deltaMh()
4537  -0.745 * deltaaMZ()
4538  +3.729 * deltaGmu() );
4539 
4540  if (FlagQuadraticTerms) {
4541  //Add contributions that are quadratic in the effective coefficients
4542  mu += 0.0;
4543  }
4544 
4545  } else if (sqrt_s == 1.4) {
4546 
4547  C1 = 0.0058;
4548 
4549  mu +=
4550  +120512. * CiHbox / LambdaNP2
4551  -4746.27 * CiHL1_11 / LambdaNP2
4552  -2212.55 * CiHe_11 / LambdaNP2
4553  -521829. * CiHL3_11 / LambdaNP2
4554  -204054. * CiHD / LambdaNP2
4555  +1891.37 * CiHB / LambdaNP2
4556  -54492.9 * CiHW / LambdaNP2
4557  -379916. * CiHWB / LambdaNP2
4558  +142.745 * CiDHB / LambdaNP2
4559  -75976. * CiDHW / LambdaNP2
4560  -4.712 * DeltaGF()
4561  -4.486 * deltaMwd6()
4562  ;
4563 
4564  // Add modifications due to small variations of the SM parameters
4565  mu += cHSM * (
4566  +5.108 * deltaMz()
4567  -0.447 * deltaMh()
4568  -0.767 * deltaaMZ()
4569  +3.751 * deltaGmu() );
4570 
4571  if (FlagQuadraticTerms) {
4572  //Add contributions that are quadratic in the effective coefficients
4573  mu += 0.0;
4574  }
4575 
4576  } else if (sqrt_s == 1.5) {
4577 
4578  C1 = 0.0058;// Use the same as 1400 GeV
4579 
4580  mu +=
4581  +120512. * CiHbox / LambdaNP2
4582  -4105.67 * CiHL1_11 / LambdaNP2
4583  -2086.49 * CiHe_11 / LambdaNP2
4584  -536150. * CiHL3_11 / LambdaNP2
4585  -204072. * CiHD / LambdaNP2
4586  +1682.65 * CiHB / LambdaNP2
4587  -53138.1 * CiHW / LambdaNP2
4588  -379943. * CiHWB / LambdaNP2
4589  +134.612 * CiDHB / LambdaNP2
4590  -78546.2 * CiDHW / LambdaNP2
4591  -4.711 * DeltaGF()
4592  -4.469 * deltaMwd6()
4593  ;
4594 
4595  // Add modifications due to small variations of the SM parameters
4596  mu += cHSM * (
4597  +5.132 * deltaMz()
4598  -0.424 * deltaMh()
4599  -0.773 * deltaaMZ()
4600  +3.757 * deltaGmu() );
4601 
4602  if (FlagQuadraticTerms) {
4603  //Add contributions that are quadratic in the effective coefficients
4604  mu += 0.0;
4605  }
4606 
4607  } else if (sqrt_s == 3.0) {
4608 
4609  C1 = 0.0057;
4610 
4611  mu +=
4612  +120404. * CiHbox / LambdaNP2
4613  -1215.14 * CiHL1_11 / LambdaNP2
4614  -1382.75 * CiHe_11 / LambdaNP2
4615  -686451. * CiHL3_11 / LambdaNP2
4616  -204039. * CiHD / LambdaNP2
4617  +293.31 * CiHB / LambdaNP2
4618  -41440.6 * CiHW / LambdaNP2
4619  -380130. * CiHWB / LambdaNP2
4620  -272.36 * CiDHB / LambdaNP2
4621  -104900. * CiDHW / LambdaNP2
4622  -4.706 * DeltaGF()
4623  -4.343 * deltaMwd6()
4624  ;
4625 
4626  // Add modifications due to small variations of the SM parameters
4627  mu += cHSM * (
4628  +5.307 * deltaMz()
4629  -0.283 * deltaMh()
4630  -0.802 * deltaaMZ()
4631  +3.789 * deltaGmu() );
4632 
4633  if (FlagQuadraticTerms) {
4634  //Add contributions that are quadratic in the effective coefficients
4635  mu += 0.0;
4636  }
4637 
4638  } else
4639  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvv()");
4640 
4641  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
4642  mu += eeeWBFint + eeeWBFpar;
4643 
4644 // Linear contribution from Higgs self-coupling
4645  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
4646 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
4648 
4649  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
4650 
4651  return mu;
4652 }

◆ mueeHvvPol()

double NPSMEFTd6::mueeHvvPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{e^+e^- \to H\nu\bar{\nu}}\)

Reimplemented from NPbase.

Definition at line 4655 of file NPSMEFTd6.cpp.

4656 {
4657  double mu = 1.0;
4658 
4659  double C1 = 0.0;
4660 
4661 // For the Higgs trilinear dependence assume the WBF mechanism dominates
4662 
4663  if (sqrt_s == 0.240) {
4664 
4665  C1 = 0.0064;
4666 
4667  if (Pol_em == 80. && Pol_ep == -30.){
4668  mu +=
4669  +121180. * CiHbox / LambdaNP2
4670  +221479. * CiHL1_11 / LambdaNP2
4671  -508958. * CiHe_11 / LambdaNP2
4672  +220003. * CiHL3_11 / LambdaNP2
4673  -149238. * CiHD / LambdaNP2
4674  +24268.3 * CiHB / LambdaNP2
4675  -32411.5 * CiHW / LambdaNP2
4676  -194663. * CiHWB / LambdaNP2
4677  +29267.1 * CiDHB / LambdaNP2
4678  -11610.1 * CiDHW / LambdaNP2
4679  -3.633 * DeltaGF()
4680  -4.394 * deltaMwd6()
4681  ;
4682 
4683  // Add modifications due to small variations of the SM parameters
4684  mu += cHSM * ( +2.975 * deltaMz()
4685  -2.624 * deltaMh()
4686  +0.379 * deltaaMZ()
4687  +2.282 * deltaGmu() );
4688 
4689  } else if (Pol_em == -80. && Pol_ep == 30.){
4690  mu +=
4691  +121456. * CiHbox / LambdaNP2
4692  +337881. * CiHL1_11 / LambdaNP2
4693  +931.718 * CiHe_11 / LambdaNP2
4694  +283908. * CiHL3_11 / LambdaNP2
4695  -199920. * CiHD / LambdaNP2
4696  -78796.8 * CiHB / LambdaNP2
4697  +34606.7 * CiHW / LambdaNP2
4698  -418335. * CiHWB / LambdaNP2
4699  -28484. * CiDHB / LambdaNP2
4700  -1197.92 * CiDHW / LambdaNP2
4701  -4.781 * DeltaGF()
4702  -5.537 * deltaMwd6()
4703  ;
4704 
4705  // Add modifications due to small variations of the SM parameters
4706  mu += cHSM * ( +5.005 * deltaMz()
4707  -2.529 * deltaMh()
4708  -0.603 * deltaaMZ()
4709  +3.57 * deltaGmu() );
4710 
4711  } else if (Pol_em == 80. && Pol_ep == 0.){
4712  mu +=
4713  +121483. * CiHbox / LambdaNP2
4714  +266382. * CiHL1_11 / LambdaNP2
4715  -313151. * CiHe_11 / LambdaNP2
4716  +245682. * CiHL3_11 / LambdaNP2
4717  -168446. * CiHD / LambdaNP2
4718  -15072.1 * CiHB / LambdaNP2
4719  -6209.98 * CiHW / LambdaNP2
4720  -281195. * CiHWB / LambdaNP2
4721  +6468.72 * CiDHB / LambdaNP2
4722  -7633.09 * CiDHW / LambdaNP2
4723  -4.079 * DeltaGF()
4724  -4.832 * deltaMwd6()
4725  ;
4726 
4727  // Add modifications due to small variations of the SM parameters
4728  mu += cHSM * ( +3.758 * deltaMz()
4729  -2.579 * deltaMh()
4730  +0.009 * deltaaMZ()
4731  +2.778 * deltaGmu() );
4732 
4733  } else if (Pol_em == -80. && Pol_ep == 0.){
4734  mu +=
4735  +121500. * CiHbox / LambdaNP2
4736  +337280. * CiHL1_11 / LambdaNP2
4737  -1209.82 * CiHe_11 / LambdaNP2
4738  +283754. * CiHL3_11 / LambdaNP2
4739  -199723. * CiHD / LambdaNP2
4740  -78465.3 * CiHB / LambdaNP2
4741  +34393.4 * CiHW / LambdaNP2
4742  -417413. * CiHWB / LambdaNP2
4743  -28344.3 * CiDHB / LambdaNP2
4744  -1296.23 * CiDHW / LambdaNP2
4745  -4.777 * DeltaGF()
4746  -5.539 * deltaMwd6()
4747  ;
4748 
4749  // Add modifications due to small variations of the SM parameters
4750  mu += cHSM * ( +4.99 * deltaMz()
4751  -2.528 * deltaMh()
4752  -0.6 * deltaaMZ()
4753  +3.56 * deltaGmu() );
4754 
4755  } else {
4756  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4757  }
4758 
4759  } else if (sqrt_s == 0.250) {
4760 
4761  C1 = 0.0064;
4762 
4763  if (Pol_em == 80. && Pol_ep == -30.){
4764  mu +=
4765  +120626. * CiHbox / LambdaNP2
4766  +172936. * CiHL1_11 / LambdaNP2
4767  -516799. * CiHe_11 / LambdaNP2
4768  +146366. * CiHL3_11 / LambdaNP2
4769  -156275. * CiHD / LambdaNP2
4770  +30993.1 * CiHB / LambdaNP2
4771  -62277.2 * CiHW / LambdaNP2
4772  -213096. * CiHWB / LambdaNP2
4773  +32593.7 * CiDHB / LambdaNP2
4774  -18479.4 * CiDHW / LambdaNP2
4775  -3.678 * DeltaGF()
4776  -4.598 * deltaMwd6()
4777  ;
4778 
4779  // Add modifications due to small variations of the SM parameters
4780  mu += cHSM * ( +2.739 * deltaMz()
4781  -2.661 * deltaMh()
4782  +0.356 * deltaaMZ()
4783  +2.343 * deltaGmu() );
4784 
4785  } else if (Pol_em == -80. && Pol_ep == 30.){
4786  mu +=
4787  +120567. * CiHbox / LambdaNP2
4788  +263666. * CiHL1_11 / LambdaNP2
4789  -351.165 * CiHe_11 / LambdaNP2
4790  -396055. * CiHL3_11 / LambdaNP2
4791  -204612. * CiHD / LambdaNP2
4792  -64672.8 * CiHB / LambdaNP2
4793  -5618.64 * CiHW / LambdaNP2
4794  -418629. * CiHWB / LambdaNP2
4795  -24815.6 * CiDHB / LambdaNP2
4796  -9013.23 * CiDHW / LambdaNP2
4797  +286902. * CiLL_1221 / LambdaNP2
4798  -5.706 * deltaMwd6()
4799  ;
4800 
4801  // Add modifications due to small variations of the SM parameters
4802  mu += cHSM * ( +4.313 * deltaMz()
4803  -2.793 * deltaMh()
4804  -0.544 * deltaaMZ()
4805  +3.494 * deltaGmu() );
4806 
4807  } else if (Pol_em == 80. && Pol_ep == 0.){
4808  mu +=
4809  +120240. * CiHbox / LambdaNP2
4810  +208124. * CiHL1_11 / LambdaNP2
4811  -315248. * CiHe_11 / LambdaNP2
4812  +158895. * CiHL3_11 / LambdaNP2
4813  -175074. * CiHD / LambdaNP2
4814  -6529.15 * CiHB / LambdaNP2
4815  -40099.4 * CiHW / LambdaNP2
4816  -293696. * CiHWB / LambdaNP2
4817  +10284.9 * CiDHB / LambdaNP2
4818  -15311.7 * CiDHW / LambdaNP2
4819  -4.092 * DeltaGF()
4820  -5.01 * deltaMwd6()
4821  ;
4822 
4823  // Add modifications due to small variations of the SM parameters
4824  mu += cHSM * ( +3.351 * deltaMz()
4825  -2.698 * deltaMh()
4826  -0.006 * deltaaMZ()
4827  +2.791 * deltaGmu() );
4828 
4829  } else if (Pol_em == -80. && Pol_ep == 0.){
4830  mu +=
4831  +120459. * CiHbox / LambdaNP2
4832  +263262. * CiHL1_11 / LambdaNP2
4833  -2507.98 * CiHe_11 / LambdaNP2
4834  +177390. * CiHL3_11 / LambdaNP2
4835  -204514. * CiHD / LambdaNP2
4836  -64371.5 * CiHB / LambdaNP2
4837  -5927.95 * CiHW / LambdaNP2
4838  -417860. * CiHWB / LambdaNP2
4839  -24699.8 * CiDHB / LambdaNP2
4840  -9119.93 * CiDHW / LambdaNP2
4841  -4.726 * DeltaGF()
4842  -5.715 * deltaMwd6()
4843  ;
4844 
4845  // Add modifications due to small variations of the SM parameters
4846  mu += cHSM * ( +4.305 * deltaMz()
4847  -2.793 * deltaMh()
4848  -0.54 * deltaaMZ()
4849  +3.492 * deltaGmu() );
4850 
4851  } else {
4852  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4853  }
4854 
4855  } else if (sqrt_s == 0.350) {
4856 
4857  C1 = 0.0062;
4858 
4859  if (Pol_em == 80. && Pol_ep == -30.){
4860  mu +=
4861  +120937. * CiHbox / LambdaNP2
4862  -41080.7 * CiHL1_11 / LambdaNP2
4863  -416801. * CiHe_11 / LambdaNP2
4864  -192794. * CiHL3_11 / LambdaNP2
4865  -182281. * CiHD / LambdaNP2
4866  +102909. * CiHB / LambdaNP2
4867  -87947.8 * CiHW / LambdaNP2
4868  -228111. * CiHWB / LambdaNP2
4869  +40181.7 * CiDHB / LambdaNP2
4870  -37530.5 * CiDHW / LambdaNP2
4871  -4.236 * DeltaGF()
4872  -4.832 * deltaMwd6()
4873  ;
4874 
4875  // Add modifications due to small variations of the SM parameters
4876  mu += cHSM * ( +3.177 * deltaMz()
4877  -1.894 * deltaMh()
4878  -0.171 * deltaaMZ()
4879  +3.022 * deltaGmu() );
4880 
4881  } else if (Pol_em == -80. && Pol_ep == 30.){
4882  mu +=
4883  +120796. * CiHbox / LambdaNP2
4884  -17710.6 * CiHL1_11 / LambdaNP2
4885  -1357.61 * CiHe_11 / LambdaNP2
4886  -241114. * CiHL3_11 / LambdaNP2
4887  -206464. * CiHD / LambdaNP2
4888  +5738.97 * CiHB / LambdaNP2
4889  -94600.4 * CiHW / LambdaNP2
4890  -387581. * CiHWB / LambdaNP2
4891  -1403.89 * CiDHB / LambdaNP2
4892  -31363.8 * CiDHW / LambdaNP2
4893  -4.699 * DeltaGF()
4894  -5.361 * deltaMwd6()
4895  ;
4896 
4897  // Add modifications due to small variations of the SM parameters
4898  mu += cHSM * ( +3.768 * deltaMz()
4899  -2. * deltaMh()
4900  -0.556 * deltaaMZ()
4901  +3.512 * deltaGmu() );
4902 
4903  } else if (Pol_em == 80. && Pol_ep == 0.){
4904  mu +=
4905  +121065. * CiHbox / LambdaNP2
4906  -30567.4 * CiHL1_11 / LambdaNP2
4907  -235832. * CiHe_11 / LambdaNP2
4908  -213581. * CiHL3_11 / LambdaNP2
4909  -192620. * CiHD / LambdaNP2
4910  +60320.1 * CiHB / LambdaNP2
4911  -90446.2 * CiHW / LambdaNP2
4912  -297833. * CiHWB / LambdaNP2
4913  +22132.1 * CiDHB / LambdaNP2
4914  -34844.4 * CiDHW / LambdaNP2
4915  -4.439 * DeltaGF()
4916  -5.054 * deltaMwd6()
4917  ;
4918 
4919  // Add modifications due to small variations of the SM parameters
4920  mu += cHSM * ( +3.437 * deltaMz()
4921  -1.943 * deltaMh()
4922  -0.343 * deltaaMZ()
4923  +3.237 * deltaGmu() );
4924 
4925  } else if (Pol_em == -80. && Pol_ep == 0.){
4926  mu +=
4927  +120725. * CiHbox / LambdaNP2
4928  -17741.9 * CiHL1_11 / LambdaNP2
4929  -2786.58 * CiHe_11 / LambdaNP2
4930  -241197. * CiHL3_11 / LambdaNP2
4931  -206387. * CiHD / LambdaNP2
4932  +6134.48 * CiHB / LambdaNP2
4933  -94603.3 * CiHW / LambdaNP2
4934  -387053. * CiHWB / LambdaNP2
4935  -1323.12 * CiDHB / LambdaNP2
4936  -31434.2 * CiDHW / LambdaNP2
4937  -4.696 * DeltaGF()
4938  -5.365 * deltaMwd6()
4939  ;
4940 
4941  // Add modifications due to small variations of the SM parameters
4942  mu += cHSM * ( +3.764 * deltaMz()
4943  -2. * deltaMh()
4944  -0.556 * deltaaMZ()
4945  +3.517 * deltaGmu() );
4946 
4947  } else {
4948  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
4949  }
4950 
4951  } else if (sqrt_s == 0.365) {
4952 
4953  C1 = 0.0062; // Use the same as 350 GeV
4954 
4955  if (Pol_em == 80. && Pol_ep == -30.){
4956  mu +=
4957  +121120. * CiHbox / LambdaNP2
4958  -43274.8 * CiHL1_11 / LambdaNP2
4959  -379332. * CiHe_11 / LambdaNP2
4960  -213151. * CiHL3_11 / LambdaNP2
4961  -185704. * CiHD / LambdaNP2
4962  +95027.9 * CiHB / LambdaNP2
4963  -87042.2 * CiHW / LambdaNP2
4964  -246839. * CiHWB / LambdaNP2
4965  +37834.6 * CiDHB / LambdaNP2
4966  -38594.2 * CiDHW / LambdaNP2
4967  -4.314 * DeltaGF()
4968  -4.867 * deltaMwd6()
4969  ;
4970 
4971  // Add modifications due to small variations of the SM parameters
4972  mu += cHSM * ( +3.356 * deltaMz()
4973  -1.787 * deltaMh()
4974  -0.246 * deltaaMZ()
4975  +3.12 * deltaGmu() );
4976 
4977  } else if (Pol_em == -80. && Pol_ep == 30.){
4978  mu +=
4979  +120708. * CiHbox / LambdaNP2
4980  -23163.4 * CiHL1_11 / LambdaNP2
4981  -1266.64 * CiHe_11 / LambdaNP2
4982  -256145. * CiHL3_11 / LambdaNP2
4983  -206112. * CiHD / LambdaNP2
4984  +7209.08 * CiHB / LambdaNP2
4985  -94095.3 * CiHW / LambdaNP2
4986  -386056. * CiHWB / LambdaNP2
4987  -673.745 * CiDHB / LambdaNP2
4988  -32528.4 * CiDHW / LambdaNP2
4989  -4.703 * DeltaGF()
4990  -5.297 * deltaMwd6()
4991  ;
4992 
4993  // Add modifications due to small variations of the SM parameters
4994  mu += cHSM * ( +3.865 * deltaMz()
4995  -1.869 * deltaMh()
4996  -0.577 * deltaaMZ()
4997  +3.533 * deltaGmu() );
4998 
4999  } else if (Pol_em == 80. && Pol_ep == 0.){
5000  mu +=
5001  +120872. * CiHbox / LambdaNP2
5002  -34492.1 * CiHL1_11 / LambdaNP2
5003  -212361. * CiHe_11 / LambdaNP2
5004  -232050. * CiHL3_11 / LambdaNP2
5005  -194801. * CiHD / LambdaNP2
5006  +56353. * CiHB / LambdaNP2
5007  -90080.9 * CiHW / LambdaNP2
5008  -308151. * CiHWB / LambdaNP2
5009  +20707.2 * CiDHB / LambdaNP2
5010  -35840.6 * CiDHW / LambdaNP2
5011  -4.485 * DeltaGF()
5012  -5.033 * deltaMwd6()
5013  ;
5014 
5015  // Add modifications due to small variations of the SM parameters
5016  mu += cHSM * ( +3.586 * deltaMz()
5017  -1.817 * deltaMh()
5018  -0.393 * deltaaMZ()
5019  +3.287 * deltaGmu() );
5020 
5021  } else if (Pol_em == -80. && Pol_ep == 0.){
5022  mu +=
5023  +120806. * CiHbox / LambdaNP2
5024  -23082.3 * CiHL1_11 / LambdaNP2
5025  -2521.89 * CiHe_11 / LambdaNP2
5026  -255807. * CiHL3_11 / LambdaNP2
5027  -205972. * CiHD / LambdaNP2
5028  +7600.7 * CiHB / LambdaNP2
5029  -94080.6 * CiHW / LambdaNP2
5030  -385587. * CiHWB / LambdaNP2
5031  -525.394 * CiDHB / LambdaNP2
5032  -32486.9 * CiDHW / LambdaNP2
5033  -4.703 * DeltaGF()
5034  -5.294 * deltaMwd6()
5035  ;
5036 
5037  // Add modifications due to small variations of the SM parameters
5038  mu += cHSM * ( +3.87 * deltaMz()
5039  -1.873 * deltaMh()
5040  -0.577 * deltaaMZ()
5041  +3.533 * deltaGmu() );
5042 
5043  } else {
5044  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5045  }
5046 
5047  } else if (sqrt_s == 0.380) {
5048 
5049  C1 = 0.0062; // Use the same as 350 GeV
5050 
5051  if (Pol_em == 80. && Pol_ep == -30.){
5052  mu +=
5053  +120907. * CiHbox / LambdaNP2
5054  -43917.7 * CiHL1_11 / LambdaNP2
5055  -344628. * CiHe_11 / LambdaNP2
5056  -230932. * CiHL3_11 / LambdaNP2
5057  -188656. * CiHD / LambdaNP2
5058  +86802.5 * CiHB / LambdaNP2
5059  -86378.3 * CiHW / LambdaNP2
5060  -262732. * CiHWB / LambdaNP2
5061  +35211.7 * CiDHB / LambdaNP2
5062  -39122. * CiDHW / LambdaNP2
5063  -4.375 * DeltaGF()
5064  -4.833 * deltaMwd6()
5065  ;
5066 
5067  // Add modifications due to small variations of the SM parameters
5068  mu += cHSM * ( +3.526 * deltaMz()
5069  -1.675 * deltaMh()
5070  -0.322 * deltaaMZ()
5071  +3.202 * deltaGmu() );
5072 
5073  } else if (Pol_em == -80. && Pol_ep == 30.){
5074  mu +=
5075  +120826. * CiHbox / LambdaNP2
5076  -26397.1 * CiHL1_11 / LambdaNP2
5077  -1156.51 * CiHe_11 / LambdaNP2
5078  -268680. * CiHL3_11 / LambdaNP2
5079  -205752. * CiHD / LambdaNP2
5080  +8226.72 * CiHB / LambdaNP2
5081  -92973.9 * CiHW / LambdaNP2
5082  -384868. * CiHWB / LambdaNP2
5083  -154.996 * CiDHB / LambdaNP2
5084  -33479.2 * CiDHW / LambdaNP2
5085  -4.706 * DeltaGF()
5086  -5.24 * deltaMwd6()
5087  ;
5088 
5089  // Add modifications due to small variations of the SM parameters
5090  mu += cHSM * ( +3.957 * deltaMz()
5091  -1.756 * deltaMh()
5092  -0.592 * deltaaMZ()
5093  +3.551 * deltaGmu() );
5094 
5095  } else if (Pol_em == 80. && Pol_ep == 0.){
5096  mu +=
5097  +121123. * CiHbox / LambdaNP2
5098  -35934.5 * CiHL1_11 / LambdaNP2
5099  -191922. * CiHe_11 / LambdaNP2
5100  -247636. * CiHL3_11 / LambdaNP2
5101  -196255. * CiHD / LambdaNP2
5102  +52143.1 * CiHB / LambdaNP2
5103  -89227.7 * CiHW / LambdaNP2
5104  -317018. * CiHWB / LambdaNP2
5105  +19725.8 * CiDHB / LambdaNP2
5106  -36723.5 * CiDHW / LambdaNP2
5107  -4.524 * DeltaGF()
5108  -5.007 * deltaMwd6()
5109  ;
5110 
5111  // Add modifications due to small variations of the SM parameters
5112  mu += cHSM * ( +3.729 * deltaMz()
5113  -1.706 * deltaMh()
5114  -0.439 * deltaaMZ()
5115  +3.366 * deltaGmu() );
5116 
5117  } else if (Pol_em == -80. && Pol_ep == 0.){
5118  mu +=
5119  +120839. * CiHbox / LambdaNP2
5120  -26545. * CiHL1_11 / LambdaNP2
5121  -2293.44 * CiHe_11 / LambdaNP2
5122  -268673. * CiHL3_11 / LambdaNP2
5123  -205696. * CiHD / LambdaNP2
5124  +8476.41 * CiHB / LambdaNP2
5125  -92899.6 * CiHW / LambdaNP2
5126  -384414. * CiHWB / LambdaNP2
5127  +15.496 * CiDHB / LambdaNP2
5128  -33502.8 * CiDHW / LambdaNP2
5129  -4.704 * DeltaGF()
5130  -5.232 * deltaMwd6()
5131  ;
5132 
5133  // Add modifications due to small variations of the SM parameters
5134  mu += cHSM * ( +3.958 * deltaMz()
5135  -1.755 * deltaMh()
5136  -0.59 * deltaaMZ()
5137  +3.555 * deltaGmu() );
5138 
5139  } else {
5140  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5141  }
5142 
5143  } else if (sqrt_s == 0.500) {
5144 
5145  C1 = 0.0061;
5146 
5147  if (Pol_em == 80. && Pol_ep == -30.){
5148  mu +=
5149  +120734. * CiHbox / LambdaNP2
5150  -33626. * CiHL1_11 / LambdaNP2
5151  -177471. * CiHe_11 / LambdaNP2
5152  -312922. * CiHL3_11 / LambdaNP2
5153  -199388. * CiHD / LambdaNP2
5154  +44288.8 * CiHB / LambdaNP2
5155  -78960.3 * CiHW / LambdaNP2
5156  -332501. * CiHWB / LambdaNP2
5157  +20615.5 * CiDHB / LambdaNP2
5158  -43923.9 * CiDHW / LambdaNP2
5159  -4.614 * DeltaGF()
5160  -4.84 * deltaMwd6()
5161  ;
5162 
5163  // Add modifications due to small variations of the SM parameters
5164  mu += cHSM * ( +4.296 * deltaMz()
5165  -1.178 * deltaMh()
5166  -0.582 * deltaaMZ()
5167  +3.535 * deltaGmu() );
5168 
5169  } else if (Pol_em == -80. && Pol_ep == 30.){
5170  mu +=
5171  +120746. * CiHbox / LambdaNP2
5172  -26369.8 * CiHL1_11 / LambdaNP2
5173  -905.141 * CiHe_11 / LambdaNP2
5174  -327709. * CiHL3_11 / LambdaNP2
5175  -204622. * CiHD / LambdaNP2
5176  +8508.33 * CiHB / LambdaNP2
5177  -82669.6 * CiHW / LambdaNP2
5178  -381185. * CiHWB / LambdaNP2
5179  +784.456 * CiDHB / LambdaNP2
5180  -41153.8 * CiDHW / LambdaNP2
5181  -4.711 * DeltaGF()
5182  -4.948 * deltaMwd6()
5183  ;
5184 
5185  // Add modifications due to small variations of the SM parameters
5186  mu += cHSM * ( +4.417 * deltaMz()
5187  -1.196 * deltaMh()
5188  -0.664 * deltaaMZ()
5189  +3.639 * deltaGmu() );
5190 
5191  } else if (Pol_em == 80. && Pol_ep == 0.){
5192  mu +=
5193  +120667. * CiHbox / LambdaNP2
5194  -30480.6 * CiHL1_11 / LambdaNP2
5195  -96672.9 * CiHe_11 / LambdaNP2
5196  -320011. * CiHL3_11 / LambdaNP2
5197  -201855. * CiHD / LambdaNP2
5198  +27690.6 * CiHB / LambdaNP2
5199  -80770. * CiHW / LambdaNP2
5200  -355060. * CiHWB / LambdaNP2
5201  +11299.4 * CiDHB / LambdaNP2
5202  -42756.5 * CiDHW / LambdaNP2
5203  -4.656 * DeltaGF()
5204  -4.875 * deltaMwd6()
5205  ;
5206 
5207  // Add modifications due to small variations of the SM parameters
5208  mu += cHSM * ( +4.345 * deltaMz()
5209  -1.186 * deltaMh()
5210  -0.621 * deltaaMZ()
5211  +3.589 * deltaGmu() );
5212 
5213  } else if (Pol_em == -80. && Pol_ep == 0.){
5214  mu +=
5215  +120715. * CiHbox / LambdaNP2
5216  -26433.4 * CiHL1_11 / LambdaNP2
5217  -1490.31 * CiHe_11 / LambdaNP2
5218  -327665. * CiHL3_11 / LambdaNP2
5219  -204644. * CiHD / LambdaNP2
5220  +8471.25 * CiHB / LambdaNP2
5221  -82673.2 * CiHW / LambdaNP2
5222  -381049. * CiHWB / LambdaNP2
5223  +862.813 * CiDHB / LambdaNP2
5224  -41179.7 * CiDHW / LambdaNP2
5225  -4.711 * DeltaGF()
5226  -4.942 * deltaMwd6()
5227  ;
5228 
5229  // Add modifications due to small variations of the SM parameters
5230  mu += cHSM * ( +4.416 * deltaMz()
5231  -1.194 * deltaMh()
5232  -0.664 * deltaaMZ()
5233  +3.64 * deltaGmu() );
5234 
5235  } else {
5236  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5237  }
5238 
5239  } else if (sqrt_s == 1.0) {
5240 
5241  C1 = 0.0059;
5242 
5243  if (Pol_em == 80. && Pol_ep == -30.){
5244  mu +=
5245  +120494. * CiHbox / LambdaNP2
5246  -9728.66 * CiHL1_11 / LambdaNP2
5247  -46166.9 * CiHe_11 / LambdaNP2
5248  -452752. * CiHL3_11 / LambdaNP2
5249  -203700. * CiHD / LambdaNP2
5250  +8561.22 * CiHB / LambdaNP2
5251  -61449.7 * CiHW / LambdaNP2
5252  -374076. * CiHWB / LambdaNP2
5253  +6473.98 * CiDHB / LambdaNP2
5254  -64032.3 * CiDHW / LambdaNP2
5255  -4.706 * DeltaGF()
5256  -4.581 * deltaMwd6()
5257  ;
5258 
5259  // Add modifications due to small variations of the SM parameters
5260  mu += cHSM * ( +4.956 * deltaMz()
5261  -0.583 * deltaMh()
5262  -0.739 * deltaaMZ()
5263  +3.723 * deltaGmu() );
5264 
5265  } else if (Pol_em == -80. && Pol_ep == 30.){
5266  mu +=
5267  +120522. * CiHbox / LambdaNP2
5268  -8881.26 * CiHL1_11 / LambdaNP2
5269  -529.908 * CiHe_11 / LambdaNP2
5270  -454326. * CiHL3_11 / LambdaNP2
5271  -204057. * CiHD / LambdaNP2
5272  +3158.25 * CiHB / LambdaNP2
5273  -61850.9 * CiHW / LambdaNP2
5274  -380114. * CiHWB / LambdaNP2
5275  +63.589 * CiDHB / LambdaNP2
5276  -63800.9 * CiDHW / LambdaNP2
5277  -4.712 * DeltaGF()
5278  -4.587 * deltaMwd6()
5279  ;
5280 
5281  // Add modifications due to small variations of the SM parameters
5282  mu += cHSM * ( +4.967 * deltaMz()
5283  -0.582 * deltaMh()
5284  -0.746 * deltaaMZ()
5285  +3.731 * deltaGmu() );
5286 
5287  } else if (Pol_em == 80. && Pol_ep == -20.){
5288  mu +=
5289  +120541. * CiHbox / LambdaNP2
5290  -9598.71 * CiHL1_11 / LambdaNP2
5291  -37435. * CiHe_11 / LambdaNP2
5292  -453118. * CiHL3_11 / LambdaNP2
5293  -203771. * CiHD / LambdaNP2
5294  +7555.11 * CiHB / LambdaNP2
5295  -61524.6 * CiHW / LambdaNP2
5296  -375155. * CiHWB / LambdaNP2
5297  +5263.81 * CiDHB / LambdaNP2
5298  -64001.7 * CiDHW / LambdaNP2
5299  -4.706 * DeltaGF()
5300  -4.589 * deltaMwd6()
5301  ;
5302 
5303  // Add modifications due to small variations of the SM parameters
5304  mu += cHSM * ( +4.959 * deltaMz()
5305  -0.583 * deltaMh()
5306  -0.741 * deltaaMZ()
5307  +3.726 * deltaGmu() );
5308 
5309  } else if (Pol_em == -80. && Pol_ep == 20.){
5310  mu +=
5311  +120482. * CiHbox / LambdaNP2
5312  -8932.26 * CiHL1_11 / LambdaNP2
5313  -597.015 * CiHe_11 / LambdaNP2
5314  -454406. * CiHL3_11 / LambdaNP2
5315  -204110. * CiHD / LambdaNP2
5316  +3145.81 * CiHB / LambdaNP2
5317  -61837. * CiHW / LambdaNP2
5318  -380115. * CiHWB / LambdaNP2
5319  +45.924 * CiDHB / LambdaNP2
5320  -63834.7 * CiDHW / LambdaNP2
5321  -4.711 * DeltaGF()
5322  -4.588 * deltaMwd6()
5323  ;
5324 
5325  // Add modifications due to small variations of the SM parameters
5326  mu += cHSM * ( +4.968 * deltaMz()
5327  -0.582 * deltaMh()
5328  -0.746 * deltaaMZ()
5329  +3.73 * deltaGmu() );
5330 
5331  } else if (Pol_em == 80. && Pol_ep == 0.){
5332  mu +=
5333  +120509. * CiHbox / LambdaNP2
5334  -9342.32 * CiHL1_11 / LambdaNP2
5335  -25028.5 * CiHe_11 / LambdaNP2
5336  -453487. * CiHL3_11 / LambdaNP2
5337  -203871. * CiHD / LambdaNP2
5338  +6021.71 * CiHB / LambdaNP2
5339  -61580. * CiHW / LambdaNP2
5340  -376790. * CiHWB / LambdaNP2
5341  +3494.08 * CiDHB / LambdaNP2
5342  -63959. * CiDHW / LambdaNP2
5343  -4.708 * DeltaGF()
5344  -4.589 * deltaMwd6()
5345  ;
5346 
5347  // Add modifications due to small variations of the SM parameters
5348  mu += cHSM * ( +4.962 * deltaMz()
5349  -0.582 * deltaMh()
5350  -0.742 * deltaaMZ()
5351  +3.726 * deltaGmu() );
5352 
5353  } else if (Pol_em == -80. && Pol_ep == 0.){
5354  mu +=
5355  +120526. * CiHbox / LambdaNP2
5356  -8927.83 * CiHL1_11 / LambdaNP2
5357  -633.766 * CiHe_11 / LambdaNP2
5358  -454337. * CiHL3_11 / LambdaNP2
5359  -204073. * CiHD / LambdaNP2
5360  +3196.39 * CiHB / LambdaNP2
5361  -61833.5 * CiHW / LambdaNP2
5362  -380094. * CiHWB / LambdaNP2
5363  +82.665 * CiDHB / LambdaNP2
5364  -63817.5 * CiDHW / LambdaNP2
5365  -4.712 * DeltaGF()
5366  -4.588 * deltaMwd6()
5367  ;
5368 
5369  // Add modifications due to small variations of the SM parameters
5370  mu += cHSM * ( +4.967 * deltaMz()
5371  -0.582 * deltaMh()
5372  -0.746 * deltaaMZ()
5373  +3.731 * deltaGmu() );
5374 
5375  } else {
5376  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5377  }
5378 
5379  } else if (sqrt_s == 1.4) {
5380 
5381  C1 = 0.0058;
5382 
5383  if (Pol_em == 80. && Pol_ep == -30.){
5384  mu +=
5385  +120516. * CiHbox / LambdaNP2
5386  -5019.36 * CiHL1_11 / LambdaNP2
5387  -29937.8 * CiHe_11 / LambdaNP2
5388  -521211. * CiHL3_11 / LambdaNP2
5389  -203908. * CiHD / LambdaNP2
5390  +4153.08 * CiHB / LambdaNP2
5391  -54219.3 * CiHW / LambdaNP2
5392  -377548. * CiHWB / LambdaNP2
5393  +4509.78 * CiDHB / LambdaNP2
5394  -76054.8 * CiDHW / LambdaNP2
5395  -4.71 * DeltaGF()
5396  -4.484 * deltaMwd6()
5397  ;
5398 
5399  // Add modifications due to small variations of the SM parameters
5400  mu += cHSM * ( +5.105 * deltaMz()
5401  -0.447 * deltaMh()
5402  -0.765 * deltaaMZ()
5403  +3.747 * deltaGmu() );
5404 
5405  } else if (Pol_em == -80. && Pol_ep == 30.){
5406  mu +=
5407  +120530. * CiHbox / LambdaNP2
5408  -4727.84 * CiHL1_11 / LambdaNP2
5409  -488.036 * CiHe_11 / LambdaNP2
5410  -521821. * CiHL3_11 / LambdaNP2
5411  -204045. * CiHD / LambdaNP2
5412  +1784.38 * CiHB / LambdaNP2
5413  -54507.5 * CiHW / LambdaNP2
5414  -380042. * CiHWB / LambdaNP2
5415  -122.009 * CiDHB / LambdaNP2
5416  -75950.5 * CiDHW / LambdaNP2
5417  -4.712 * DeltaGF()
5418  -4.487 * deltaMwd6()
5419  ;
5420 
5421  // Add modifications due to small variations of the SM parameters
5422  mu += cHSM * ( +5.108 * deltaMz()
5423  -0.447 * deltaMh()
5424  -0.768 * deltaaMZ()
5425  +3.749 * deltaGmu() );
5426 
5427  } else if (Pol_em == 80. && Pol_ep == 0.){
5428  mu +=
5429  +120542. * CiHbox / LambdaNP2
5430  -4870.22 * CiHL1_11 / LambdaNP2
5431  -16376.8 * CiHe_11 / LambdaNP2
5432  -521472. * CiHL3_11 / LambdaNP2
5433  -203960. * CiHD / LambdaNP2
5434  +3068.42 * CiHB / LambdaNP2
5435  -54375.2 * CiHW / LambdaNP2
5436  -378699. * CiHWB / LambdaNP2
5437  +2390.51 * CiDHB / LambdaNP2
5438  -75996.8 * CiDHW / LambdaNP2
5439  -4.711 * DeltaGF()
5440  -4.485 * deltaMwd6()
5441  ;
5442 
5443  // Add modifications due to small variations of the SM parameters
5444  mu += cHSM * ( +5.107 * deltaMz()
5445  -0.448 * deltaMh()
5446  -0.766 * deltaaMZ()
5447  +3.749 * deltaGmu() );
5448 
5449  } else if (Pol_em == -80. && Pol_ep == 0.){
5450  mu +=
5451  +120504. * CiHbox / LambdaNP2
5452  -4718.66 * CiHL1_11 / LambdaNP2
5453  -574.963 * CiHe_11 / LambdaNP2
5454  -521805. * CiHL3_11 / LambdaNP2
5455  -204053. * CiHD / LambdaNP2
5456  +1784.37 * CiHB / LambdaNP2
5457  -54482.7 * CiHW / LambdaNP2
5458  -380051. * CiHWB / LambdaNP2
5459  -99.132 * CiDHB / LambdaNP2
5460  -75974.5 * CiDHW / LambdaNP2
5461  -4.712 * DeltaGF()
5462  -4.487 * deltaMwd6()
5463  ;
5464 
5465  // Add modifications due to small variations of the SM parameters
5466  mu += cHSM * ( +5.107 * deltaMz()
5467  -0.447 * deltaMh()
5468  -0.767 * deltaaMZ()
5469  +3.749 * deltaGmu() );
5470 
5471  } else {
5472  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5473  }
5474 
5475  } else if (sqrt_s == 1.5) {
5476 
5477  C1 = 0.0058;// Use the same as 1400 GeV
5478 
5479  if (Pol_em == 80. && Pol_ep == -30.){
5480  mu +=
5481  +120531. * CiHbox / LambdaNP2
5482  -4421.38 * CiHL1_11 / LambdaNP2
5483  -28114.2 * CiHe_11 / LambdaNP2
5484  -535633. * CiHL3_11 / LambdaNP2
5485  -203960. * CiHD / LambdaNP2
5486  +3556.32 * CiHB / LambdaNP2
5487  -52816.2 * CiHW / LambdaNP2
5488  -377932. * CiHWB / LambdaNP2
5489  +4253.17 * CiDHB / LambdaNP2
5490  -78599.6 * CiDHW / LambdaNP2
5491  -4.71 * DeltaGF()
5492  -4.465 * deltaMwd6()
5493  ;
5494 
5495  // Add modifications due to small variations of the SM parameters
5496  mu += cHSM * ( +5.128 * deltaMz()
5497  -0.424 * deltaMh()
5498  -0.772 * deltaaMZ()
5499  +3.755 * deltaGmu() );
5500 
5501  } else if (Pol_em == -80. && Pol_ep == 30.){
5502  mu +=
5503  +120491. * CiHbox / LambdaNP2
5504  -4113.21 * CiHL1_11 / LambdaNP2
5505  -517.747 * CiHe_11 / LambdaNP2
5506  -536169. * CiHL3_11 / LambdaNP2
5507  -204050. * CiHD / LambdaNP2
5508  +1553.24 * CiHB / LambdaNP2
5509  -53097.9 * CiHW / LambdaNP2
5510  -380055. * CiHWB / LambdaNP2
5511  -129.437 * CiDHB / LambdaNP2
5512  -78539.4 * CiDHW / LambdaNP2
5513  -4.711 * DeltaGF()
5514  -4.468 * deltaMwd6()
5515  ;
5516 
5517  // Add modifications due to small variations of the SM parameters
5518  mu += cHSM * ( +5.131 * deltaMz()
5519  -0.424 * deltaMh()
5520  -0.773 * deltaaMZ()
5521  +3.755 * deltaGmu() );
5522 
5523  } else if (Pol_em == 80. && Pol_ep == 0.){
5524  mu +=
5525  +120525. * CiHbox / LambdaNP2
5526  -4256.39 * CiHL1_11 / LambdaNP2
5527  -15376.9 * CiHe_11 / LambdaNP2
5528  -535845. * CiHL3_11 / LambdaNP2
5529  -203987. * CiHD / LambdaNP2
5530  +2641.32 * CiHB / LambdaNP2
5531  -53045.1 * CiHW / LambdaNP2
5532  -378920. * CiHWB / LambdaNP2
5533  +2237.55 * CiDHB / LambdaNP2
5534  -78549.8 * CiDHW / LambdaNP2
5535  -4.711 * DeltaGF()
5536  -4.468 * deltaMwd6()
5537  ;
5538 
5539  // Add modifications due to small variations of the SM parameters
5540  mu += cHSM * ( +5.129 * deltaMz()
5541  -0.424 * deltaMh()
5542  -0.772 * deltaaMZ()
5543  +3.753 * deltaGmu() );
5544 
5545  } else if (Pol_em == -80. && Pol_ep == 0.){
5546  mu +=
5547  +120499. * CiHbox / LambdaNP2
5548  -4113.23 * CiHL1_11 / LambdaNP2
5549  -616.984 * CiHe_11 / LambdaNP2
5550  -536155. * CiHL3_11 / LambdaNP2
5551  -204035. * CiHD / LambdaNP2
5552  +1570.5 * CiHB / LambdaNP2
5553  -53079.3 * CiHW / LambdaNP2
5554  -380043. * CiHWB / LambdaNP2
5555  -112.179 * CiDHB / LambdaNP2
5556  -78543.9 * CiDHW / LambdaNP2
5557  -4.711 * DeltaGF()
5558  -4.468 * deltaMwd6()
5559  ;
5560 
5561  // Add modifications due to small variations of the SM parameters
5562  mu += cHSM * ( +5.13 * deltaMz()
5563  -0.424 * deltaMh()
5564  -0.773 * deltaaMZ()
5565  +3.755 * deltaGmu() );
5566 
5567  } else {
5568  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5569  }
5570 
5571  } else if (sqrt_s == 3.0) {
5572 
5573  C1 = 0.0057;
5574 
5575  if (Pol_em == 80. && Pol_ep == -30.){
5576  mu +=
5577  +120384. * CiHbox / LambdaNP2
5578  -1301.85 * CiHL1_11 / LambdaNP2
5579  -16370.4 * CiHe_11 / LambdaNP2
5580  -686389. * CiHL3_11 / LambdaNP2
5581  -204031. * CiHD / LambdaNP2
5582  +628.479 * CiHB / LambdaNP2
5583  -41464.7 * CiHW / LambdaNP2
5584  -379766. * CiHWB / LambdaNP2
5585  +2259.53 * CiDHB / LambdaNP2
5586  -104941. * CiDHW / LambdaNP2
5587  -4.706 * DeltaGF()
5588  -4.342 * deltaMwd6()
5589  ;
5590 
5591  // Add modifications due to small variations of the SM parameters
5592  mu += cHSM * ( +5.306 * deltaMz()
5593  -0.283 * deltaMh()
5594  -0.802 * deltaaMZ()
5595  +3.787 * deltaGmu() );
5596 
5597  } else if (Pol_em == -80. && Pol_ep == 30.){
5598  mu +=
5599  +120423. * CiHbox / LambdaNP2
5600  -1253.47 * CiHL1_11 / LambdaNP2
5601  -537.201 * CiHe_11 / LambdaNP2
5602  -686427. * CiHL3_11 / LambdaNP2
5603  -204047. * CiHD / LambdaNP2
5604  +268.601 * CiHB / LambdaNP2
5605  -41454. * CiHW / LambdaNP2
5606  -380141. * CiHWB / LambdaNP2
5607  -447.668 * CiDHB / LambdaNP2
5608  -104906. * CiDHW / LambdaNP2
5609  -4.707 * DeltaGF()
5610  -4.342 * deltaMwd6()
5611  ;
5612 
5613  // Add modifications due to small variations of the SM parameters
5614  mu += cHSM * ( +5.305 * deltaMz()
5615  -0.284 * deltaMh()
5616  -0.802 * deltaaMZ()
5617  +3.787 * deltaGmu() );
5618 
5619  } else if (Pol_em == 80. && Pol_ep == 0.){
5620  mu +=
5621  +120399. * CiHbox / LambdaNP2
5622  -1267.47 * CiHL1_11 / LambdaNP2
5623  -9008.44 * CiHe_11 / LambdaNP2
5624  -686485. * CiHL3_11 / LambdaNP2
5625  -204052. * CiHD / LambdaNP2
5626  +439.947 * CiHB / LambdaNP2
5627  -41459.8 * CiHW / LambdaNP2
5628  -379947. * CiHWB / LambdaNP2
5629  +1005.59 * CiDHB / LambdaNP2
5630  -104927. * CiDHW / LambdaNP2
5631  -4.706 * DeltaGF()
5632  -4.342 * deltaMwd6()
5633  ;
5634 
5635  // Add modifications due to small variations of the SM parameters
5636  mu += cHSM * ( +5.303 * deltaMz()
5637  -0.283 * deltaMh()
5638  -0.802 * deltaaMZ()
5639  +3.789 * deltaGmu() );
5640 
5641  } else if (Pol_em == -80. && Pol_ep == 0.){
5642  mu +=
5643  +120385. * CiHbox / LambdaNP2
5644  -1245.4 * CiHL1_11 / LambdaNP2
5645  -535.407 * CiHe_11 / LambdaNP2
5646  -686461. * CiHL3_11 / LambdaNP2
5647  -204048. * CiHD / LambdaNP2
5648  +244.425 * CiHB / LambdaNP2
5649  -41447.5 * CiHW / LambdaNP2
5650  -380150. * CiHWB / LambdaNP2
5651  -430.653 * CiDHB / LambdaNP2
5652  -104905. * CiDHW / LambdaNP2
5653  -4.706 * DeltaGF()
5654  -4.343 * deltaMwd6()
5655  ;
5656 
5657  // Add modifications due to small variations of the SM parameters
5658  mu += cHSM * ( +5.307 * deltaMz()
5659  -0.283 * deltaMh()
5660  -0.802 * deltaaMZ()
5661  +3.789 * deltaGmu() );
5662 
5663  } else {
5664  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5665  }
5666 
5667  } else
5668  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeHvvPol()");
5669 
5670  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
5671  mu += eeeWBFint + eeeWBFpar;
5672 
5673 // Linear contribution from Higgs self-coupling
5674  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
5675 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
5677 
5678  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
5679 
5680  return mu;
5681 }

◆ mueettH()

double NPSMEFTd6::mueettH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eettH}\)

Reimplemented from NPbase.

Definition at line 9329 of file NPSMEFTd6.cpp.

9330 {
9331  double mu = 1.0;
9332 
9333  double C1 = 0.0;
9334 
9335  if (sqrt_s == 0.500) {
9336 
9337  C1 = 0.086;
9338 
9339  mu +=
9340  +121901. * CiHbox / LambdaNP2
9341  +84038.2 * CiHL1_11 / LambdaNP2
9342  +41671.2 * CiHe_11 / LambdaNP2
9343  -31418.2 * CiHu_11 / LambdaNP2
9344  +84038.2 * CiHL3_11 / LambdaNP2
9345  -121791. * CiuH_33r / LambdaNP2
9346  -59467.6 * CiHD / LambdaNP2
9347  +138929. * CiHB / LambdaNP2
9348  +130909. * CiHW / LambdaNP2
9349  -253030. * CiHWB / LambdaNP2
9350  -1757.66 * CiDHB / LambdaNP2
9351  +1501.34 * CiDHW / LambdaNP2
9352  +1386027. * CiuW_33r / LambdaNP2
9353  +1698012. * CiuB_33r / LambdaNP2
9354  -1.965 * DeltaGF()
9355  -1.187 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9356  ;
9357 
9358  // Add modifications due to small variations of the SM parameters
9359  mu += cHSM * ( +1.932 * deltaMz()
9360  -9.827 * deltaMh()
9361  +1.04 * deltaaMZ()
9362  +1.992 * deltaGmu()
9363  -18.476 * deltamt() );
9364 
9365  if (FlagQuadraticTerms) {
9366  //Add contributions that are quadratic in the effective coefficients
9367  mu += 0.0;
9368  }
9369 
9370  } else if (sqrt_s == 1.0) {
9371 
9372  C1 = 0.017;
9373 
9374  mu +=
9375  +122013. * CiHbox / LambdaNP2
9376  +889282. * CiHL1_11 / LambdaNP2
9377  -543424. * CiHe_11 / LambdaNP2
9378  -8240.83 * CiHu_11 / LambdaNP2
9379  +889282. * CiHL3_11 / LambdaNP2
9380  -116099. * CiuH_33r / LambdaNP2
9381  -60351.9 * CiHD / LambdaNP2
9382  +352804. * CiHB / LambdaNP2
9383  +361918. * CiHW / LambdaNP2
9384  -397547. * CiHWB / LambdaNP2
9385  +37326.1 * CiDHB / LambdaNP2
9386  +113772. * CiDHW / LambdaNP2
9387  +2758980. * CiuW_33r / LambdaNP2
9388  +3462941. * CiuB_33r / LambdaNP2
9389  -2.08 * DeltaGF()
9390  -2.575 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9391  ;
9392 
9393  // Add modifications due to small variations of the SM parameters
9394  mu += cHSM * ( +2.185 * deltaMz()
9395  -1.195 * deltaMh()
9396  +0.92 * deltaaMZ()
9397  +2.096 * deltaGmu()
9398  +2.136 * deltamt() );
9399 
9400  if (FlagQuadraticTerms) {
9401  //Add contributions that are quadratic in the effective coefficients
9402  mu += 0.0;
9403  }
9404 
9405  } else if (sqrt_s == 1.4) {
9406 
9407  C1 = 0.0094;
9408 
9409  mu +=
9410  +122081. * CiHbox / LambdaNP2
9411  +2544832. * CiHL1_11 / LambdaNP2
9412  -1901938. * CiHe_11 / LambdaNP2
9413  +3241.73 * CiHu_11 / LambdaNP2
9414  +2544832. * CiHL3_11 / LambdaNP2
9415  -112208. * CiuH_33r / LambdaNP2
9416  -60340.4 * CiHD / LambdaNP2
9417  +464967. * CiHB / LambdaNP2
9418  +487659. * CiHW / LambdaNP2
9419  -471053. * CiHWB / LambdaNP2
9420  +134900. * CiDHB / LambdaNP2
9421  +371767. * CiDHW / LambdaNP2
9422  +3804096. * CiuW_33r / LambdaNP2
9423  +4800265. * CiuB_33r / LambdaNP2
9424  -2.139 * DeltaGF()
9425  -3.203 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9426  ;
9427 
9428  // Add modifications due to small variations of the SM parameters
9429  mu += cHSM * ( +2.309 * deltaMz()
9430  -0.898 * deltaMh()
9431  +0.872 * deltaaMZ()
9432  +2.157 * deltaGmu()
9433  +2.262 * deltamt() );
9434 
9435  if (FlagQuadraticTerms) {
9436  //Add contributions that are quadratic in the effective coefficients
9437  mu += 0.0;
9438  }
9439 
9440  } else if (sqrt_s == 1.5) {
9441 
9442  C1 = 0.0094;// Use the same as 1400 GeV
9443 
9444  mu +=
9445  +122173. * CiHbox / LambdaNP2
9446  +3117293. * CiHL1_11 / LambdaNP2
9447  -2378233. * CiHe_11 / LambdaNP2
9448  +5531.15 * CiHu_11 / LambdaNP2
9449  +3117293. * CiHL3_11 / LambdaNP2
9450  -111274. * CiuH_33r / LambdaNP2
9451  -60192. * CiHD / LambdaNP2
9452  +487962. * CiHB / LambdaNP2
9453  +513503. * CiHW / LambdaNP2
9454  -485782. * CiHWB / LambdaNP2
9455  +170734. * CiDHB / LambdaNP2
9456  +462665. * CiDHW / LambdaNP2
9457  +4068326. * CiuW_33r / LambdaNP2
9458  +5138930. * CiuB_33r / LambdaNP2
9459  -2.149 * DeltaGF()
9460  -3.325 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9461  ;
9462 
9463  // Add modifications due to small variations of the SM parameters
9464  mu += cHSM * ( +2.322 * deltaMz()
9465  -0.858 * deltaMh()
9466  +0.866 * deltaaMZ()
9467  +2.164 * deltaGmu()
9468  +2.265 * deltamt() );
9469 
9470  if (FlagQuadraticTerms) {
9471  //Add contributions that are quadratic in the effective coefficients
9472  mu += 0.0;
9473  }
9474 
9475  } else if (sqrt_s == 3.0) {
9476 
9477  C1 = 0.0037;
9478 
9479  mu +=
9480  +121915. * CiHbox / LambdaNP2
9481  +19529668. * CiHL1_11 / LambdaNP2
9482  -16356276. * CiHe_11 / LambdaNP2
9483  +23142.9 * CiHu_11 / LambdaNP2
9484  +19529668. * CiHL3_11 / LambdaNP2
9485  -104011. * CiuH_33r / LambdaNP2
9486  -58710.4 * CiHD / LambdaNP2
9487  +697868. * CiHB / LambdaNP2
9488  +751003. * CiHW / LambdaNP2
9489  -625171. * CiHWB / LambdaNP2
9490  +1204441. * CiDHB / LambdaNP2
9491  +3111413. * CiDHW / LambdaNP2
9492  +8604912. * CiuW_33r / LambdaNP2
9493  +10946841. * CiuB_33r / LambdaNP2
9494  -2.224 * DeltaGF()
9495  -4.279 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9496  ;
9497 
9498  // Add modifications due to small variations of the SM parameters
9499  mu += cHSM * ( +2.483 * deltaMz()
9500  -0.572 * deltaMh()
9501  +0.771 * deltaaMZ()
9502  +2.242 * deltaGmu()
9503  +2.182 * deltamt() );
9504 
9505  if (FlagQuadraticTerms) {
9506  //Add contributions that are quadratic in the effective coefficients
9507  mu += 0.0;
9508  }
9509 
9510  } else
9511  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettH()");
9512 
9513  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
9514  mu += eeettHint + eeettHpar;
9515 
9516 // Linear contribution from Higgs self-coupling
9517  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
9518 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
9520 
9521  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9522 
9523  return mu;
9524 }

◆ mueettHPol()

double NPSMEFTd6::mueettHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eettH}\)

Reimplemented from NPbase.

Definition at line 9526 of file NPSMEFTd6.cpp.

9527 {
9528  double mu = 1.0;
9529 
9530  double C1 = 0.0;
9531 
9532  if (sqrt_s == 0.500) {
9533 
9534  C1 = 0.086;
9535 
9536  if (Pol_em == 80. && Pol_ep == -30.){
9537  mu +=
9538  +121861. * CiHbox / LambdaNP2
9539  +14207.9 * CiHL1_11 / LambdaNP2
9540  +124191. * CiHe_11 / LambdaNP2
9541  +112591. * CiHu_11 / LambdaNP2
9542  +14207.9 * CiHL3_11 / LambdaNP2
9543  -123399. * CiuH_33r / LambdaNP2
9544  -12437.7 * CiHD / LambdaNP2
9545  +249779. * CiHB / LambdaNP2
9546  +18912.8 * CiHW / LambdaNP2
9547  -109936. * CiHWB / LambdaNP2
9548  -5170.73 * CiDHB / LambdaNP2
9549  +3167.65 * CiDHW / LambdaNP2
9550  +174267. * CiuW_33r / LambdaNP2
9551  +3032981. * CiuB_33r / LambdaNP2
9552  -0.388 * DeltaGF()
9553  +3.51 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9554  ;
9555 
9556  // Add modifications due to small variations of the SM parameters
9557  mu += cHSM * ( -1.319 * deltaMz()
9558  -9.866 * deltaMh()
9559  +2.617 * deltaaMZ()
9560  +0.421 * deltaGmu()
9561  -18.44 * deltamt() );
9562 
9563  } else if (Pol_em == -80. && Pol_ep == 30.){
9564  mu +=
9565  +121809. * CiHbox / LambdaNP2
9566  +116253. * CiHL1_11 / LambdaNP2
9567  +3415.4 * CiHe_11 / LambdaNP2
9568  -98311.8 * CiHu_11 / LambdaNP2
9569  +116253. * CiHL3_11 / LambdaNP2
9570  -121117. * CiuH_33r / LambdaNP2
9571  -81321.2 * CiHD / LambdaNP2
9572  +87352.2 * CiHB / LambdaNP2
9573  +182702. * CiHW / LambdaNP2
9574  -319427. * CiHWB / LambdaNP2
9575  -21.616 * CiDHB / LambdaNP2
9576  +799.81 * CiDHW / LambdaNP2
9577  +1948272. * CiuW_33r / LambdaNP2
9578  +1078489. * CiuB_33r / LambdaNP2
9579  -2.697 * DeltaGF()
9580  -3.37 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9581  ;
9582 
9583  // Add modifications due to small variations of the SM parameters
9584  mu += cHSM * ( +3.441 * deltaMz()
9585  -9.806 * deltaMh()
9586  +0.308 * deltaaMZ()
9587  +2.725 * deltaGmu()
9588  -18.491 * deltamt() );
9589 
9590  } else if (Pol_em == 80. && Pol_ep == 0.){
9591  mu +=
9592  +121837. * CiHbox / LambdaNP2
9593  +24323.6 * CiHL1_11 / LambdaNP2
9594  +111998. * CiHe_11 / LambdaNP2
9595  +91391.1 * CiHu_11 / LambdaNP2
9596  +24323.6 * CiHL3_11 / LambdaNP2
9597  -123203. * CiuH_33r / LambdaNP2
9598  -19404.2 * CiHD / LambdaNP2
9599  +233452. * CiHB / LambdaNP2
9600  +35310.2 * CiHW / LambdaNP2
9601  -131019. * CiHWB / LambdaNP2
9602  -4810.06 * CiDHB / LambdaNP2
9603  +2842.31 * CiDHW / LambdaNP2
9604  +351790. * CiuW_33r / LambdaNP2
9605  +2837005. * CiuB_33r / LambdaNP2
9606  -0.617 * DeltaGF()
9607  +2.818 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9608  ;
9609 
9610  // Add modifications due to small variations of the SM parameters
9611  mu += cHSM * ( -0.843 * deltaMz()
9612  -9.86 * deltaMh()
9613  +2.385 * deltaaMZ()
9614  +0.645 * deltaGmu()
9615  -18.45 * deltamt() );
9616 
9617  } else if (Pol_em == -80. && Pol_ep == 0.){
9618  mu +=
9619  +121814. * CiHbox / LambdaNP2
9620  +113858. * CiHL1_11 / LambdaNP2
9621  +6221.44 * CiHe_11 / LambdaNP2
9622  -93321.6 * CiHu_11 / LambdaNP2
9623  +113858. * CiHL3_11 / LambdaNP2
9624  -121180. * CiuH_33r / LambdaNP2
9625  -79695. * CiHD / LambdaNP2
9626  +91201.9 * CiHB / LambdaNP2
9627  +178853. * CiHW / LambdaNP2
9628  -314513. * CiHWB / LambdaNP2
9629  -137.642 * CiDHB / LambdaNP2
9630  +853.383 * CiDHW / LambdaNP2
9631  +1906734. * CiuW_33r / LambdaNP2
9632  +1124181. * CiuB_33r / LambdaNP2
9633  -2.642 * DeltaGF()
9634  -3.21 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9635  ;
9636 
9637  // Add modifications due to small variations of the SM parameters
9638  mu += cHSM * ( +3.33 * deltaMz()
9639  -9.807 * deltaMh()
9640  +0.362 * deltaaMZ()
9641  +2.671 * deltaGmu()
9642  -18.489 * deltamt() );
9643 
9644  } else {
9645  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9646  }
9647 
9648  } else if (sqrt_s == 1.0) {
9649 
9650  C1 = 0.017;
9651 
9652  if (Pol_em == 80. && Pol_ep == -30.){
9653  mu +=
9654  +122269. * CiHbox / LambdaNP2
9655  +148925. * CiHL1_11 / LambdaNP2
9656  -1516295. * CiHe_11 / LambdaNP2
9657  +181376. * CiHu_11 / LambdaNP2
9658  +148925. * CiHL3_11 / LambdaNP2
9659  -115721. * CiuH_33r / LambdaNP2
9660  -9966.97 * CiHD / LambdaNP2
9661  +648027. * CiHB / LambdaNP2
9662  +58990.6 * CiHW / LambdaNP2
9663  -166947. * CiHWB / LambdaNP2
9664  +258446. * CiDHB / LambdaNP2
9665  +27641. * CiDHW / LambdaNP2
9666  +416063. * CiuW_33r / LambdaNP2
9667  +5771745. * CiuB_33r / LambdaNP2
9668  -0.426 * DeltaGF()
9669  +3.026 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9670  ;
9671 
9672  // Add modifications due to small variations of the SM parameters
9673  mu += cHSM * ( -1.159 * deltaMz()
9674  -1.211 * deltaMh()
9675  +2.586 * deltaaMZ()
9676  +0.445 * deltaGmu()
9677  +2.101 * deltamt() );
9678 
9679  } else if (Pol_em == -80. && Pol_ep == 30.){
9680  mu +=
9681  +122212. * CiHbox / LambdaNP2
9682  +1266376. * CiHL1_11 / LambdaNP2
9683  -47326.8 * CiHe_11 / LambdaNP2
9684  -104685. * CiHu_11 / LambdaNP2
9685  +1266376. * CiHL3_11 / LambdaNP2
9686  -116193. * CiuH_33r / LambdaNP2
9687  -85861. * CiHD / LambdaNP2
9688  +202732. * CiHB / LambdaNP2
9689  +516612. * CiHW / LambdaNP2
9690  -514723. * CiHWB / LambdaNP2
9691  -75504.5 * CiDHB / LambdaNP2
9692  +158356. * CiDHW / LambdaNP2
9693  +3954267. * CiuW_33r / LambdaNP2
9694  +2288387. * CiuB_33r / LambdaNP2
9695  -2.929 * DeltaGF()
9696  -5.432 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9697  ;
9698 
9699  // Add modifications due to small variations of the SM parameters
9700  mu += cHSM * ( +3.902 * deltaMz()
9701  -1.192 * deltaMh()
9702  +0.075 * deltaaMZ()
9703  +2.94 * deltaGmu()
9704  +2.16 * deltamt() );
9705 
9706  } else if (Pol_em == 80. && Pol_ep == -20.){
9707  mu +=
9708  +122563. * CiHbox / LambdaNP2
9709  +179718. * CiHL1_11 / LambdaNP2
9710  -1476392. * CiHe_11 / LambdaNP2
9711  +173910. * CiHu_11 / LambdaNP2
9712  +179718. * CiHL3_11 / LambdaNP2
9713  -115349. * CiuH_33r / LambdaNP2
9714  -11797.8 * CiHD / LambdaNP2
9715  +636347. * CiHB / LambdaNP2
9716  +71703.6 * CiHW / LambdaNP2
9717  -176417. * CiHWB / LambdaNP2
9718  +249649. * CiDHB / LambdaNP2
9719  +31542.3 * CiDHW / LambdaNP2
9720  +513357. * CiuW_33r / LambdaNP2
9721  +5678281. * CiuB_33r / LambdaNP2
9722  -0.497 * DeltaGF()
9723  +2.823 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9724  ;
9725 
9726  // Add modifications due to small variations of the SM parameters
9727  mu += cHSM * ( -0.986 * deltaMz()
9728  -1.242 * deltaMh()
9729  +2.514 * deltaaMZ()
9730  +0.529 * deltaGmu()
9731  +2.133 * deltamt() );
9732 
9733  } else if (Pol_em == -80. && Pol_ep == 20.){
9734  mu +=
9735  +122316. * CiHbox / LambdaNP2
9736  +1258544. * CiHL1_11 / LambdaNP2
9737  -57807.1 * CiHe_11 / LambdaNP2
9738  -102560. * CiHu_11 / LambdaNP2
9739  +1258544. * CiHL3_11 / LambdaNP2
9740  -116091. * CiuH_33r / LambdaNP2
9741  -85249.7 * CiHD / LambdaNP2
9742  +206295. * CiHB / LambdaNP2
9743  +513404. * CiHW / LambdaNP2
9744  -512197. * CiHWB / LambdaNP2
9745  -72925.9 * CiDHB / LambdaNP2
9746  +157286. * CiDHW / LambdaNP2
9747  +3929488. * CiuW_33r / LambdaNP2
9748  +2314064. * CiuB_33r / LambdaNP2
9749  -2.911 * DeltaGF()
9750  -5.37 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9751  ;
9752 
9753  // Add modifications due to small variations of the SM parameters
9754  mu += cHSM * ( +3.877 * deltaMz()
9755  -1.222 * deltaMh()
9756  +0.099 * deltaaMZ()
9757  +2.937 * deltaGmu()
9758  +2.184 * deltamt() );
9759 
9760  } else if (Pol_em == 80. && Pol_ep == 0.){
9761  mu +=
9762  +122564. * CiHbox / LambdaNP2
9763  +252265. * CiHL1_11 / LambdaNP2
9764  -1381101. * CiHe_11 / LambdaNP2
9765  +155161. * CiHu_11 / LambdaNP2
9766  +252265. * CiHL3_11 / LambdaNP2
9767  -115358. * CiuH_33r / LambdaNP2
9768  -16813.1 * CiHD / LambdaNP2
9769  +607466. * CiHB / LambdaNP2
9770  +101359. * CiHW / LambdaNP2
9771  -198737. * CiHWB / LambdaNP2
9772  +227834. * CiDHB / LambdaNP2
9773  +39939.6 * CiDHW / LambdaNP2
9774  +742520. * CiuW_33r / LambdaNP2
9775  +5453267. * CiuB_33r / LambdaNP2
9776  -0.659 * DeltaGF()
9777  +2.273 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9778  ;
9779 
9780  // Add modifications due to small variations of the SM parameters
9781  mu += cHSM * ( -0.69 * deltaMz()
9782  -1.205 * deltaMh()
9783  +2.349 * deltaaMZ()
9784  +0.676 * deltaGmu()
9785  +2.105 * deltamt() );
9786 
9787  } else if (Pol_em == -80. && Pol_ep == 0.){
9788  mu +=
9789  +122380. * CiHbox / LambdaNP2
9790  +1238124. * CiHL1_11 / LambdaNP2
9791  -84811.2 * CiHe_11 / LambdaNP2
9792  -97259.2 * CiHu_11 / LambdaNP2
9793  +1238124. * CiHL3_11 / LambdaNP2
9794  -116044. * CiuH_33r / LambdaNP2
9795  -83798.9 * CiHD / LambdaNP2
9796  +214128. * CiHB / LambdaNP2
9797  +505118. * CiHW / LambdaNP2
9798  -505830. * CiHWB / LambdaNP2
9799  -66814.1 * CiDHB / LambdaNP2
9800  +155075. * CiDHW / LambdaNP2
9801  +3863710. * CiuW_33r / LambdaNP2
9802  +2378351. * CiuB_33r / LambdaNP2
9803  -2.867 * DeltaGF()
9804  -5.212 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9805  ;
9806 
9807  // Add modifications due to small variations of the SM parameters
9808  mu += cHSM * ( +3.771 * deltaMz()
9809  -1.195 * deltaMh()
9810  +0.137 * deltaaMZ()
9811  +2.878 * deltaGmu()
9812  +2.166 * deltamt() );
9813 
9814  } else {
9815  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9816  }
9817 
9818  } else if (sqrt_s == 1.4) {
9819 
9820  C1 = 0.0094;
9821 
9822  if (Pol_em == 80. && Pol_ep == -30.){
9823  mu +=
9824  +121945. * CiHbox / LambdaNP2
9825  +416437. * CiHL1_11 / LambdaNP2
9826  -5198451. * CiHe_11 / LambdaNP2
9827  +211446. * CiHu_11 / LambdaNP2
9828  +416437. * CiHL3_11 / LambdaNP2
9829  -110413. * CiuH_33r / LambdaNP2
9830  -8089.5 * CiHD / LambdaNP2
9831  +852065. * CiHB / LambdaNP2
9832  +78915.7 * CiHW / LambdaNP2
9833  -191411. * CiHWB / LambdaNP2
9834  +881670. * CiDHB / LambdaNP2
9835  +72289.2 * CiDHW / LambdaNP2
9836  +588296. * CiuW_33r / LambdaNP2
9837  +7812392. * CiuB_33r / LambdaNP2
9838  -0.441 * DeltaGF()
9839  +2.819 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9840  ;
9841 
9842  // Add modifications due to small variations of the SM parameters
9843  mu += cHSM * ( -1.109 * deltaMz()
9844  -0.905 * deltaMh()
9845  +2.571 * deltaaMZ()
9846  +0.451 * deltaGmu()
9847  +2.225 * deltamt() );
9848 
9849  } else if (Pol_em == -80. && Pol_ep == 30.){
9850  mu +=
9851  +122124. * CiHbox / LambdaNP2
9852  +3668482. * CiHL1_11 / LambdaNP2
9853  -164738. * CiHe_11 / LambdaNP2
9854  -106285. * CiHu_11 / LambdaNP2
9855  +3668482. * CiHL3_11 / LambdaNP2
9856  -112775. * CiuH_33r / LambdaNP2
9857  -87497.2 * CiHD / LambdaNP2
9858  +261266. * CiHB / LambdaNP2
9859  +703789. * CiHW / LambdaNP2
9860  -618584. * CiHWB / LambdaNP2
9861  -257636. * CiDHB / LambdaNP2
9862  +530202. * CiDHW / LambdaNP2
9863  +5501929. * CiuW_33r / LambdaNP2
9864  +3213842. * CiuB_33r / LambdaNP2
9865  -3.038 * DeltaGF()
9866  -6.378 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9867  ;
9868 
9869  // Add modifications due to small variations of the SM parameters
9870  mu += cHSM * ( +4.12 * deltaMz()
9871  -0.898 * deltaMh()
9872  -0.029 * deltaaMZ()
9873  +3.056 * deltaGmu()
9874  +2.28 * deltamt() );
9875 
9876  } else if (Pol_em == 80. && Pol_ep == 0.){
9877  mu +=
9878  +121843. * CiHbox / LambdaNP2
9879  +706068. * CiHL1_11 / LambdaNP2
9880  -4748505. * CiHe_11 / LambdaNP2
9881  +182964. * CiHu_11 / LambdaNP2
9882  +706068. * CiHL3_11 / LambdaNP2
9883  -110672. * CiuH_33r / LambdaNP2
9884  -15249.5 * CiHD / LambdaNP2
9885  +798771. * CiHB / LambdaNP2
9886  +134415. * CiHW / LambdaNP2
9887  -229663. * CiHWB / LambdaNP2
9888  +779863. * CiDHB / LambdaNP2
9889  +112951. * CiDHW / LambdaNP2
9890  +1026697. * CiuW_33r / LambdaNP2
9891  +7402171. * CiuB_33r / LambdaNP2
9892  -0.673 * DeltaGF()
9893  +1.996 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9894  ;
9895 
9896  // Add modifications due to small variations of the SM parameters
9897  mu += cHSM * ( -0.648 * deltaMz()
9898  -0.901 * deltaMh()
9899  +2.34 * deltaaMZ()
9900  +0.693 * deltaGmu()
9901  +2.232 * deltamt() );
9902 
9903  } else if (Pol_em == -80. && Pol_ep == 0.){
9904  mu +=
9905  +122069. * CiHbox / LambdaNP2
9906  +3581543. * CiHL1_11 / LambdaNP2
9907  -298692. * CiHe_11 / LambdaNP2
9908  -97874.3 * CiHu_11 / LambdaNP2
9909  +3581543. * CiHL3_11 / LambdaNP2
9910  -112737. * CiuH_33r / LambdaNP2
9911  -85431.2 * CiHD / LambdaNP2
9912  +276629. * CiHB / LambdaNP2
9913  +687136. * CiHW / LambdaNP2
9914  -607155. * CiHWB / LambdaNP2
9915  -227375. * CiDHB / LambdaNP2
9916  +517945. * CiDHW / LambdaNP2
9917  +5370183. * CiuW_33r / LambdaNP2
9918  +3335906. * CiuB_33r / LambdaNP2
9919  -2.969 * DeltaGF()
9920  -6.138 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9921  ;
9922 
9923  // Add modifications due to small variations of the SM parameters
9924  mu += cHSM * ( +3.976 * deltaMz()
9925  -0.895 * deltaMh()
9926  +0.039 * deltaaMZ()
9927  +2.986 * deltaGmu()
9928  +2.271 * deltamt() );
9929 
9930  } else {
9931  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
9932  }
9933 
9934  } else if (sqrt_s == 1.5) {
9935 
9936  C1 = 0.0094;// Use the same as 1400 GeV
9937 
9938  if (Pol_em == 80. && Pol_ep == -30.){
9939  mu +=
9940  +121854. * CiHbox / LambdaNP2
9941  +507190. * CiHL1_11 / LambdaNP2
9942  -6475118. * CiHe_11 / LambdaNP2
9943  +216935. * CiHu_11 / LambdaNP2
9944  +507190. * CiHL3_11 / LambdaNP2
9945  -109820. * CiuH_33r / LambdaNP2
9946  -7568.59 * CiHD / LambdaNP2
9947  +893094. * CiHB / LambdaNP2
9948  +82781.5 * CiHW / LambdaNP2
9949  -196556. * CiHWB / LambdaNP2
9950  +1099527. * CiDHB / LambdaNP2
9951  +87228. * CiDHW / LambdaNP2
9952  +630747. * CiuW_33r / LambdaNP2
9953  +8328477. * CiuB_33r / LambdaNP2
9954  -0.442 * DeltaGF()
9955  +2.756 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9956  ;
9957 
9958  // Add modifications due to small variations of the SM parameters
9959  mu += cHSM * ( -1.104 * deltaMz()
9960  -0.856 * deltaMh()
9961  +2.568 * deltaaMZ()
9962  +0.455 * deltaGmu()
9963  +2.232 * deltamt() );
9964 
9965  } else if (Pol_em == -80. && Pol_ep == 30.){
9966  mu +=
9967  +121994. * CiHbox / LambdaNP2
9968  +4501280. * CiHL1_11 / LambdaNP2
9969  -206085. * CiHe_11 / LambdaNP2
9970  -106381. * CiHu_11 / LambdaNP2
9971  +4501280. * CiHL3_11 / LambdaNP2
9972  -112104. * CiuH_33r / LambdaNP2
9973  -87805.6 * CiHD / LambdaNP2
9974  +273106. * CiHB / LambdaNP2
9975  +741955. * CiHW / LambdaNP2
9976  -639545. * CiHWB / LambdaNP2
9977  -322155. * CiDHB / LambdaNP2
9978  +661931. * CiDHW / LambdaNP2
9979  +5892414. * CiuW_33r / LambdaNP2
9980  +3448015. * CiuB_33r / LambdaNP2
9981  -3.057 * DeltaGF()
9982  -6.552 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
9983  ;
9984 
9985  // Add modifications due to small variations of the SM parameters
9986  mu += cHSM * ( +4.154 * deltaMz()
9987  -0.856 * deltaMh()
9988  -0.045 * deltaaMZ()
9989  +3.071 * deltaGmu()
9990  +2.287 * deltamt() );
9991 
9992  } else if (Pol_em == 80. && Pol_ep == 0.){
9993  mu +=
9994  +121793. * CiHbox / LambdaNP2
9995  +861242. * CiHL1_11 / LambdaNP2
9996  -5919951. * CiHe_11 / LambdaNP2
9997  +188249. * CiHu_11 / LambdaNP2
9998  +861242. * CiHL3_11 / LambdaNP2
9999  -109696. * CiuH_33r / LambdaNP2
10000  -14806.7 * CiHD / LambdaNP2
10001  +837632. * CiHB / LambdaNP2
10002  +141142. * CiHW / LambdaNP2
10003  -235907. * CiHWB / LambdaNP2
10004  +973107. * CiDHB / LambdaNP2
10005  +138331. * CiDHW / LambdaNP2
10006  +1097452. * CiuW_33r / LambdaNP2
10007  +7895510. * CiuB_33r / LambdaNP2
10008  -0.673 * DeltaGF()
10009  +1.935 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
10010  ;
10011 
10012  // Add modifications due to small variations of the SM parameters
10013  mu += cHSM * ( -0.637 * deltaMz()
10014  -0.859 * deltaMh()
10015  +2.339 * deltaaMZ()
10016  +0.68 * deltaGmu()
10017  +2.236 * deltamt() );
10018 
10019  } else if (Pol_em == -80. && Pol_ep == 0.){
10020  mu +=
10021  +122029. * CiHbox / LambdaNP2
10022  +4394189. * CiHL1_11 / LambdaNP2
10023  -373205. * CiHe_11 / LambdaNP2
10024  -97750.6 * CiHu_11 / LambdaNP2
10025  +4394189. * CiHL3_11 / LambdaNP2
10026  -112024. * CiuH_33r / LambdaNP2
10027  -85643.3 * CiHD / LambdaNP2
10028  +289620. * CiHB / LambdaNP2
10029  +724463. * CiHW / LambdaNP2
10030  -627885. * CiHWB / LambdaNP2
10031  -284076. * CiDHB / LambdaNP2
10032  +646658. * CiDHW / LambdaNP2
10033  +5753330. * CiuW_33r / LambdaNP2
10034  +3578793. * CiuB_33r / LambdaNP2
10035  -2.989 * DeltaGF()
10036  -6.311 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
10037  ;
10038 
10039  // Add modifications due to small variations of the SM parameters
10040  mu += cHSM * ( +4.014 * deltaMz()
10041  -0.855 * deltaMh()
10042  +0.024 * deltaaMZ()
10043  +3.011 * deltaGmu()
10044  +2.286 * deltamt() );
10045 
10046  } else {
10047  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
10048  }
10049 
10050  } else if (sqrt_s == 3.0) {
10051 
10052  C1 = 0.0037;
10053 
10054  if (Pol_em == 80. && Pol_ep == -30.){
10055  mu +=
10056  +122442. * CiHbox / LambdaNP2
10057  +3092340. * CiHL1_11 / LambdaNP2
10058  -43264264. * CiHe_11 / LambdaNP2
10059  +259622. * CiHu_11 / LambdaNP2
10060  +3092340. * CiHL3_11 / LambdaNP2
10061  -100510. * CiuH_33r / LambdaNP2
10062  -3230.01 * CiHD / LambdaNP2
10063  +1267548. * CiHB / LambdaNP2
10064  +118886. * CiHW / LambdaNP2
10065  -247164. * CiHWB / LambdaNP2
10066  +7397753. * CiDHB / LambdaNP2
10067  +510206. * CiDHW / LambdaNP2
10068  +1343630. * CiuW_33r / LambdaNP2
10069  +17234081. * CiuB_33r / LambdaNP2
10070  -0.459 * DeltaGF()
10071  +2.453 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
10072  ;
10073 
10074  // Add modifications due to small variations of the SM parameters
10075  mu += cHSM * ( -1.07 * deltaMz()
10076  -0.576 * deltaMh()
10077  +2.542 * deltaaMZ()
10078  +0.468 * deltaGmu()
10079  +2.145 * deltamt() );
10080 
10081  } else if (Pol_em == -80. && Pol_ep == 30.){
10082  mu +=
10083  +122230. * CiHbox / LambdaNP2
10084  +28686134. * CiHL1_11 / LambdaNP2
10085  -1435177. * CiHe_11 / LambdaNP2
10086  -108195. * CiHu_11 / LambdaNP2
10087  +28686134. * CiHL3_11 / LambdaNP2
10088  -105858. * CiuH_33r / LambdaNP2
10089  -89803.1 * CiHD / LambdaNP2
10090  +381886. * CiHB / LambdaNP2
10091  +1102843. * CiHW / LambdaNP2
10092  -834821. * CiHWB / LambdaNP2
10093  -2237555. * CiDHB / LambdaNP2
10094  +4557030. * CiDHW / LambdaNP2
10095  +12639913. * CiuW_33r / LambdaNP2
10096  +7455995. * CiuB_33r / LambdaNP2
10097  -3.212 * DeltaGF()
10098  -8.009 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
10099  ;
10100 
10101  // Add modifications due to small variations of the SM parameters
10102  mu += cHSM * ( +4.469 * deltaMz()
10103  -0.595 * deltaMh()
10104  -0.222 * deltaaMZ()
10105  +3.22 * deltaGmu()
10106  +2.195 * deltamt() );
10107 
10108  } else if (Pol_em == 80. && Pol_ep == 0.){
10109  mu +=
10110  +122688. * CiHbox / LambdaNP2
10111  +5271741. * CiHL1_11 / LambdaNP2
10112  -39707692. * CiHe_11 / LambdaNP2
10113  +228729. * CiHu_11 / LambdaNP2
10114  +5271741. * CiHL3_11 / LambdaNP2
10115  -100891. * CiuH_33r / LambdaNP2
10116  -10526.3 * CiHD / LambdaNP2
10117  +1192421. * CiHB / LambdaNP2
10118  +202915. * CiHW / LambdaNP2
10119  -296939. * CiHWB / LambdaNP2
10120  +6582510. * CiDHB / LambdaNP2
10121  +853895. * CiDHW / LambdaNP2
10122  +2303644. * CiuW_33r / LambdaNP2
10123  +16407287. * CiuB_33r / LambdaNP2
10124  -0.693 * DeltaGF()
10125  +1.565 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
10126  ;
10127 
10128  // Add modifications due to small variations of the SM parameters
10129  mu += cHSM * ( -0.597 * deltaMz()
10130  -0.565 * deltaMh()
10131  +2.305 * deltaaMZ()
10132  +0.708 * deltaGmu()
10133  +2.153 * deltamt() );
10134 
10135  } else if (Pol_em == -80. && Pol_ep == 0.){
10136  mu +=
10137  +121781. * CiHbox / LambdaNP2
10138  +27966374. * CiHL1_11 / LambdaNP2
10139  -2597153. * CiHe_11 / LambdaNP2
10140  -98089.4 * CiHu_11 / LambdaNP2
10141  +27966374. * CiHL3_11 / LambdaNP2
10142  -105885. * CiuH_33r / LambdaNP2
10143  -87600.3 * CiHD / LambdaNP2
10144  +406305. * CiHB / LambdaNP2
10145  +1075086. * CiHW / LambdaNP2
10146  -818808. * CiHWB / LambdaNP2
10147  -1967062. * CiDHB / LambdaNP2
10148  +4442109. * CiDHW / LambdaNP2
10149  +12322125. * CiuW_33r / LambdaNP2
10150  +7728315. * CiuB_33r / LambdaNP2
10151  -3.134 * DeltaGF()
10152  -7.724 * 0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
10153  ;
10154 
10155  // Add modifications due to small variations of the SM parameters
10156  mu += cHSM * ( +4.305 * deltaMz()
10157  -0.59 * deltaMh()
10158  -0.147 * deltaaMZ()
10159  +3.144 * deltaGmu()
10160  +2.192 * deltamt() );
10161 
10162  } else {
10163  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
10164  }
10165 
10166  } else
10167  throw std::runtime_error("Bad argument in NPSMEFTd6::mueettHPol()");
10168 
10169  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
10170  mu += eeettHint + eeettHpar;
10171 
10172 // Linear contribution from Higgs self-coupling
10173  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
10174 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
10176 
10177  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
10178 
10179  return mu;
10180 }

◆ mueeWBF()

double NPSMEFTd6::mueeWBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeWBF}\)

Reimplemented from NPbase.

Definition at line 4018 of file NPSMEFTd6.cpp.

4019 {
4020  double mu = 1.0;
4021 
4022  double C1 = 0.0;
4023 
4024  if (sqrt_s == 0.240) {
4025 
4026  C1 = 0.0064;
4027 
4028  mu +=
4029  +121120. * CiHbox / LambdaNP2
4030  -138682. * CiHL3_11 / LambdaNP2
4031  -203727. * CiHD / LambdaNP2
4032  -24699.7 * CiHW / LambdaNP2
4033  -379830. * CiHWB / LambdaNP2
4034  -18173.7 * CiDHW / LambdaNP2
4035  -4.716 * DeltaGF()
4036  -5.665 * deltaMwd6()
4037  ;
4038 
4039  // Add modifications due to small variations of the SM parameters
4040  mu += cHSM * (
4041  +3.307 * deltaMz()
4042  -3.995 * deltaMh()
4043  -0.486 * deltaaMZ()
4044  +3.507 * deltaGmu() );
4045 
4046  if (FlagQuadraticTerms) {
4047  //Add contributions that are quadratic in the effective coefficients
4048  mu += 0.0;
4049  }
4050 
4051  } else if (sqrt_s == 0.250) {
4052 
4053  C1 = 0.0064;
4054 
4055  mu +=
4056  +121142. * CiHbox / LambdaNP2
4057  -147357. * CiHL3_11 / LambdaNP2
4058  -203726. * CiHD / LambdaNP2
4059  -26559.2 * CiHW / LambdaNP2
4060  -379797. * CiHWB / LambdaNP2
4061  -19265.3 * CiDHW / LambdaNP2
4062  -4.717 * DeltaGF()
4063  -5.593 * deltaMwd6()
4064  ;
4065 
4066  // Add modifications due to small variations of the SM parameters
4067  mu += cHSM * (
4068  +3.413 * deltaMz()
4069  -3.644 * deltaMh()
4070  -0.502 * deltaaMZ()
4071  +3.523 * deltaGmu() );
4072 
4073  if (FlagQuadraticTerms) {
4074  //Add contributions that are quadratic in the effective coefficients
4075  mu += 0.0;
4076  }
4077 
4078  } else if (sqrt_s == 0.350) {
4079 
4080  C1 = 0.0062;
4081 
4082  mu +=
4083  +121107. * CiHbox / LambdaNP2
4084  -219582. * CiHL3_11 / LambdaNP2
4085  -203717. * CiHD / LambdaNP2
4086  -39722.3 * CiHW / LambdaNP2
4087  -379795. * CiHWB / LambdaNP2
4088  -28864.2 * CiDHW / LambdaNP2
4089  -4.714 * DeltaGF()
4090  -5.13 * deltaMwd6()
4091  ;
4092 
4093  // Add modifications due to small variations of the SM parameters
4094  mu += cHSM * (
4095  +4.073 * deltaMz()
4096  -1.94 * deltaMh()
4097  -0.598 * deltaaMZ()
4098  +3.623 * deltaGmu() );
4099 
4100  if (FlagQuadraticTerms) {
4101  //Add contributions that are quadratic in the effective coefficients
4102  mu += 0.0;
4103  }
4104 
4105  } else if (sqrt_s == 0.365) {
4106 
4107  C1 = 0.0062; // Use the same as 350 GeV
4108 
4109  mu +=
4110  +121071. * CiHbox / LambdaNP2
4111  -228452. * CiHL3_11 / LambdaNP2
4112  -203725. * CiHD / LambdaNP2
4113  -40966.9 * CiHW / LambdaNP2
4114  -379798. * CiHWB / LambdaNP2
4115  -30110.4 * CiDHW / LambdaNP2
4116  -4.714 * DeltaGF()
4117  -5.08 * deltaMwd6()
4118  ;
4119 
4120  // Add modifications due to small variations of the SM parameters
4121  mu += cHSM * (
4122  +4.136 * deltaMz()
4123  -1.817 * deltaMh()
4124  -0.609 * deltaaMZ()
4125  +3.635 * deltaGmu() );
4126 
4127  if (FlagQuadraticTerms) {
4128  //Add contributions that are quadratic in the effective coefficients
4129  mu += 0.0;
4130  }
4131 
4132  } else if (sqrt_s == 0.380) {
4133 
4134  C1 = 0.0062; // Use the same as 350 GeV
4135 
4136  mu +=
4137  +121001. * CiHbox / LambdaNP2
4138  -237126. * CiHL3_11 / LambdaNP2
4139  -203726. * CiHD / LambdaNP2
4140  -42070.9 * CiHW / LambdaNP2
4141  -379788. * CiHWB / LambdaNP2
4142  -31352.7 * CiDHW / LambdaNP2
4143  -4.714 * DeltaGF()
4144  -5.044 * deltaMwd6()
4145  ;
4146 
4147  // Add modifications due to small variations of the SM parameters
4148  mu += cHSM * (
4149  +4.192 * deltaMz()
4150  -1.711 * deltaMh()
4151  -0.618 * deltaaMZ()
4152  +3.64 * deltaGmu() );
4153 
4154  if (FlagQuadraticTerms) {
4155  //Add contributions that are quadratic in the effective coefficients
4156  mu += 0.0;
4157  }
4158 
4159  } else if (sqrt_s == 0.500) {
4160 
4161  C1 = 0.0061;
4162 
4163  mu +=
4164  +121063. * CiHbox / LambdaNP2
4165  -295115. * CiHL3_11 / LambdaNP2
4166  -203679. * CiHD / LambdaNP2
4167  -47539.5 * CiHW / LambdaNP2
4168  -379773. * CiHWB / LambdaNP2
4169  -39825.1 * CiDHW / LambdaNP2
4170  -4.715 * DeltaGF()
4171  -4.817 * deltaMwd6()
4172  ;
4173 
4174  // Add modifications due to small variations of the SM parameters
4175  mu += cHSM * (
4176  +4.509 * deltaMz()
4177  -1.178 * deltaMh()
4178  -0.666 * deltaaMZ()
4179  +3.692 * deltaGmu() );
4180 
4181  if (FlagQuadraticTerms) {
4182  //Add contributions that are quadratic in the effective coefficients
4183  mu += 0.0;
4184  }
4185 
4186  } else if (sqrt_s == 1.0) {
4187 
4188  C1 = 0.0059;
4189 
4190  mu +=
4191  +120960. * CiHbox / LambdaNP2
4192  -442647. * CiHL3_11 / LambdaNP2
4193  -203748. * CiHD / LambdaNP2
4194  -49375.4 * CiHW / LambdaNP2
4195  -379685. * CiHWB / LambdaNP2
4196  -63503.9 * CiDHW / LambdaNP2
4197  -4.712 * DeltaGF()
4198  -4.481 * deltaMwd6()
4199  ;
4200 
4201  // Add modifications due to small variations of the SM parameters
4202  mu += cHSM * (
4203  +4.99 * deltaMz()
4204  -0.582 * deltaMh()
4205  -0.734 * deltaaMZ()
4206  +3.765 * deltaGmu() );
4207 
4208  if (FlagQuadraticTerms) {
4209  //Add contributions that are quadratic in the effective coefficients
4210  mu += 0.0;
4211  }
4212 
4213  } else if (sqrt_s == 1.4) {
4214 
4215  C1 = 0.0058;
4216 
4217  mu +=
4218  +121118. * CiHbox / LambdaNP2
4219  -515189. * CiHL3_11 / LambdaNP2
4220  -203684. * CiHD / LambdaNP2
4221  -46619.5 * CiHW / LambdaNP2
4222  -379667. * CiHWB / LambdaNP2
4223  -75747.8 * CiDHW / LambdaNP2
4224  -4.714 * DeltaGF()
4225  -4.391 * deltaMwd6()
4226  ;
4227 
4228  // Add modifications due to small variations of the SM parameters
4229  mu += cHSM * (
4230  +5.13 * deltaMz()
4231  -0.446 * deltaMh()
4232  -0.754 * deltaaMZ()
4233  +3.784 * deltaGmu() );
4234 
4235  if (FlagQuadraticTerms) {
4236  //Add contributions that are quadratic in the effective coefficients
4237  mu += 0.0;
4238  }
4239 
4240  } else if (sqrt_s == 1.5) {
4241 
4242  C1 = 0.0058;// Use the same as 1400 GeV
4243 
4244  mu +=
4245  +121200. * CiHbox / LambdaNP2
4246  -530152. * CiHL3_11 / LambdaNP2
4247  -203649. * CiHD / LambdaNP2
4248  -45921.3 * CiHW / LambdaNP2
4249  -379591. * CiHWB / LambdaNP2
4250  -78241.3 * CiDHW / LambdaNP2
4251  -4.715 * DeltaGF()
4252  -4.38 * deltaMwd6()
4253  ;
4254 
4255  // Add modifications due to small variations of the SM parameters
4256  mu += cHSM * (
4257  +5.154 * deltaMz()
4258  -0.424 * deltaMh()
4259  -0.757 * deltaaMZ()
4260  +3.786 * deltaGmu() );
4261 
4262  if (FlagQuadraticTerms) {
4263  //Add contributions that are quadratic in the effective coefficients
4264  mu += 0.0;
4265  }
4266 
4267  } else if (sqrt_s == 3.0) {
4268 
4269  C1 = 0.0057;
4270 
4271  mu +=
4272  +121321. * CiHbox / LambdaNP2
4273  -684382. * CiHL3_11 / LambdaNP2
4274  -203585. * CiHD / LambdaNP2
4275  -38239. * CiHW / LambdaNP2
4276  -379518. * CiHWB / LambdaNP2
4277  -104465. * CiDHW / LambdaNP2
4278  -4.714 * DeltaGF()
4279  -4.258 * deltaMwd6()
4280  ;
4281 
4282  // Add modifications due to small variations of the SM parameters
4283  mu += cHSM * (
4284  +5.331 * deltaMz()
4285  -0.279 * deltaMh()
4286  -0.785 * deltaaMZ()
4287  +3.81 * deltaGmu() );
4288 
4289  if (FlagQuadraticTerms) {
4290  //Add contributions that are quadratic in the effective coefficients
4291  mu += 0.0;
4292  }
4293 
4294  } else
4295  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWBF()");
4296 
4297  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
4298  mu += eeeWBFint + eeeWBFpar;
4299 
4300 // Linear contribution from Higgs self-coupling
4301  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
4302 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
4304 
4305  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
4306 
4307  return mu;
4308 }

◆ mueeWBFPol()

double NPSMEFTd6::mueeWBFPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeWBF}\)

Reimplemented from NPbase.

Definition at line 4311 of file NPSMEFTd6.cpp.

4312 {
4313 
4314 // Pure WBF, hence only initiated by LH fermions. No difference between polarizations at the linear level.
4315 // Expand like other functions when quadratic terms are included
4316 
4317  return mueeWBF(sqrt_s);
4318 }

◆ mueeWW()

double NPSMEFTd6::mueeWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeWW}\)

Reimplemented from NPbase.

Definition at line 14239 of file NPSMEFTd6.cpp.

14240 {
14241  double mu = 1.0;
14242 
14243  if (sqrt_s == 0.161) {
14244 
14245  mu +=
14246  -127.685 * CiHL1_11 / LambdaNP2
14247  -175.567 * CiHe_11 / LambdaNP2
14248  +242506. * CiHL3_11 / LambdaNP2
14249  -86570.7 * CiHD / LambdaNP2
14250  -189772. * CiHWB / LambdaNP2
14251  +12.769 * CiDHB / LambdaNP2
14252  +6.384 * CiDHW / LambdaNP2
14253  +0. * CiW / LambdaNP2
14254  -2.858 * DeltaGF()
14255  -70.01 * deltaMwd6();
14256 
14257  // Add modifications due to small variations of the SM parameters
14258  mu += cHSM * ( -13.134 * deltaMz()
14259  +0. * deltaaMZ()
14260  +18.795 * deltaGmu() );
14261 
14262  if (FlagQuadraticTerms) {
14263  //Add contributions that are quadratic in the effective coefficients
14264  mu += 0.0;
14265  }
14266 
14267  } else if (sqrt_s == 0.240) {
14268 
14269  mu +=
14270  -26882.4 * CiHL1_11 / LambdaNP2
14271  -17485.4 * CiHe_11 / LambdaNP2
14272  +267456. * CiHL3_11 / LambdaNP2
14273  -83799.2 * CiHD / LambdaNP2
14274  -168074. * CiHWB / LambdaNP2
14275  +3199.72 * CiDHB / LambdaNP2
14276  +3401.93 * CiDHW / LambdaNP2
14277  +6649.22 * CiW / LambdaNP2
14278  -2.812 * DeltaGF()
14279  -0.993 * deltaMwd6();
14280 
14281  // Add modifications due to small variations of the SM parameters
14282  mu += cHSM * ( +4.101 * deltaMz()
14283  -0.584 * deltaaMZ()
14284  +2.688 * deltaGmu() );
14285 
14286  if (FlagQuadraticTerms) {
14287  //Add contributions that are quadratic in the effective coefficients
14288  mu += 0.0;
14289  }
14290 
14291  } else if (sqrt_s == 0.250) {
14292 
14293  mu +=
14294  -29442.7 * CiHL1_11 / LambdaNP2
14295  -18494.5 * CiHe_11 / LambdaNP2
14296  +269747. * CiHL3_11 / LambdaNP2
14297  -83750.9 * CiHD / LambdaNP2
14298  -167811. * CiHWB / LambdaNP2
14299  +3401.99 * CiDHB / LambdaNP2
14300  +3624.67 * CiDHW / LambdaNP2
14301  +7249.33 * CiW / LambdaNP2
14302  -2.812 * DeltaGF()
14303  -0.959 * deltaMwd6();
14304 
14305  // Add modifications due to small variations of the SM parameters
14306  mu += cHSM * ( +4.184 * deltaMz()
14307  -0.585 * deltaaMZ()
14308  +2.709 * deltaGmu() );
14309 
14310  if (FlagQuadraticTerms) {
14311  //Add contributions that are quadratic in the effective coefficients
14312  mu += 0.0;
14313  }
14314 
14315  } else if (sqrt_s == 0.350) {
14316 
14317  mu +=
14318  -47552.4 * CiHL1_11 / LambdaNP2
14319  -23798.8 * CiHe_11 / LambdaNP2
14320  +289379. * CiHL3_11 / LambdaNP2
14321  -83905.3 * CiHD / LambdaNP2
14322  -168326. * CiHWB / LambdaNP2
14323  +5979.05 * CiDHB / LambdaNP2
14324  +6520.95 * CiDHW / LambdaNP2
14325  +10476.9 * CiW / LambdaNP2
14326  -2.832 * DeltaGF()
14327  -0.781 * deltaMwd6();
14328 
14329  // Add modifications due to small variations of the SM parameters
14330  mu += cHSM * ( +4.516 * deltaMz()
14331  -0.659 * deltaaMZ()
14332  +2.768 * deltaGmu());
14333 
14334  if (FlagQuadraticTerms) {
14335  //Add contributions that are quadratic in the effective coefficients
14336  mu += 0.0;
14337  }
14338 
14339  } else if (sqrt_s == 0.365) {
14340 
14341  mu +=
14342  -49800.4 * CiHL1_11 / LambdaNP2
14343  -24520.1 * CiHe_11 / LambdaNP2
14344  +290743. * CiHL3_11 / LambdaNP2
14345  -84033.5 * CiHD / LambdaNP2
14346  -168466. * CiHWB / LambdaNP2
14347  +6310.59 * CiDHB / LambdaNP2
14348  +6842.81 * CiDHW / LambdaNP2
14349  +10606.3 * CiW / LambdaNP2
14350  -2.828 * DeltaGF()
14351  -0.775 * deltaMwd6();
14352 
14353  // Add modifications due to small variations of the SM parameters
14354  mu += cHSM * ( +4.533 * deltaMz()
14355  -0.661 * deltaaMZ()
14356  +2.789 * deltaGmu() );
14357 
14358  if (FlagQuadraticTerms) {
14359  //Add contributions that are quadratic in the effective coefficients
14360  mu += 0.0;
14361  }
14362 
14363  } else if (sqrt_s == 0.500) {
14364 
14365  mu +=
14366  -68234.1 * CiHL1_11 / LambdaNP2
14367  -31290. * CiHe_11 / LambdaNP2
14368  +309504. * CiHL3_11 / LambdaNP2
14369  -84926.8 * CiHD / LambdaNP2
14370  -171658. * CiHWB / LambdaNP2
14371  +9325.19 * CiDHB / LambdaNP2
14372  +10009.9 * CiDHW / LambdaNP2
14373  +10896.4 * CiW / LambdaNP2
14374  -2.84 * DeltaGF()
14375  -0.705 * deltaMwd6();
14376 
14377  // Add modifications due to small variations of the SM parameters
14378  mu += cHSM * ( +4.7 * deltaMz()
14379  -0.683 * deltaaMZ()
14380  +2.799 * deltaGmu() );
14381 
14382  if (FlagQuadraticTerms) {
14383  //Add contributions that are quadratic in the effective coefficients
14384  mu += 0.0;
14385  }
14386 
14387  } else
14388  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWW()");
14389 
14390  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
14391 
14392  return mu;
14393 }

◆ mueeWWPol()

double NPSMEFTd6::mueeWWPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeWW}\)

Reimplemented from NPbase.

Definition at line 14396 of file NPSMEFTd6.cpp.

14397 {
14398  double mu = 1.0;
14399 
14400  if (sqrt_s == 0.240) {
14401 
14402  if (Pol_em == 80. && Pol_ep == -30.){
14403  mu +=
14404  -23395. * CiHL1_11 / LambdaNP2
14405  -261092. * CiHe_11 / LambdaNP2
14406  +231526. * CiHL3_11 / LambdaNP2
14407  -72645.8 * CiHD / LambdaNP2
14408  -25084.5 * CiHWB / LambdaNP2
14409  +27060.4 * CiDHB / LambdaNP2
14410  -7822.83 * CiDHW / LambdaNP2
14411  -587.63 * CiW / LambdaNP2
14412  -2.437 * DeltaGF()
14413  -1.554 * deltaMwd6();
14414 
14415  // Add modifications due to small variations of the SM parameters
14416  mu += cHSM * ( +3.226 * deltaMz()
14417  -0.083 * deltaaMZ()
14418  +2.189 * deltaGmu() );
14419 
14420  } else if (Pol_em == -80. && Pol_ep == 30.){
14421  mu +=
14422  -27334.5 * CiHL1_11 / LambdaNP2
14423  -564.392 * CiHe_11 / LambdaNP2
14424  +269600. * CiHL3_11 / LambdaNP2
14425  -84684.5 * CiHD / LambdaNP2
14426  -178168. * CiHWB / LambdaNP2
14427  +1539.25 * CiDHB / LambdaNP2
14428  +4130.32 * CiDHW / LambdaNP2
14429  +7121.6 * CiW / LambdaNP2
14430  -2.838 * DeltaGF()
14431  -0.949 * deltaMwd6();
14432 
14433  // Add modifications due to small variations of the SM parameters
14434  mu += cHSM * ( +4.156 * deltaMz()
14435  -0.607 * deltaaMZ()
14436  +2.724 * deltaGmu() );
14437 
14438  } else {
14439  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14440  }
14441 
14442  } else if (sqrt_s == 0.250) {
14443 
14444  if (Pol_em == 80. && Pol_ep == -30.){
14445  mu +=
14446  -25554.9 * CiHL1_11 / LambdaNP2
14447  -274633. * CiHe_11 / LambdaNP2
14448  +234621. * CiHL3_11 / LambdaNP2
14449  -72498.3 * CiHD / LambdaNP2
14450  -23308.5 * CiHWB / LambdaNP2
14451  +29321.9 * CiDHB / LambdaNP2
14452  -7518.62 * CiDHW / LambdaNP2
14453  +314.876 * CiW / LambdaNP2
14454  -2.444 * DeltaGF()
14455  -1.448 * deltaMwd6();
14456 
14457  // Add modifications due to small variations of the SM parameters
14458  mu += cHSM * ( +3.37 * deltaMz()
14459  -0.119 * deltaaMZ()
14460  +2.223 * deltaGmu() );
14461 
14462  } else if (Pol_em == -80. && Pol_ep == 30.){
14463  mu +=
14464  -29714.6 * CiHL1_11 / LambdaNP2
14465  -693.518 * CiHe_11 / LambdaNP2
14466  +271032. * CiHL3_11 / LambdaNP2
14467  -84929.3 * CiHD / LambdaNP2
14468  -177727. * CiHWB / LambdaNP2
14469  +1648.44 * CiDHB / LambdaNP2
14470  +4443.85 * CiDHW / LambdaNP2
14471  +7778.07 * CiW / LambdaNP2
14472  -2.829 * DeltaGF()
14473  -0.914 * deltaMwd6();
14474 
14475  // Add modifications due to small variations of the SM parameters
14476  mu += cHSM * ( +4.233 * deltaMz()
14477  -0.62 * deltaaMZ()
14478  +2.73 * deltaGmu() );
14479 
14480  } else if (Pol_em == 80. && Pol_ep == 0.){
14481  mu +=
14482  -27418.7 * CiHL1_11 / LambdaNP2
14483  -157891. * CiHe_11 / LambdaNP2
14484  +250086. * CiHL3_11 / LambdaNP2
14485  -77904.2 * CiHD / LambdaNP2
14486  -89451.9 * CiHWB / LambdaNP2
14487  +17499.7 * CiDHB / LambdaNP2
14488  -2499.14 * CiDHW / LambdaNP2
14489  +3435.6 * CiW / LambdaNP2
14490  -2.607 * DeltaGF()
14491  -1.242 * deltaMwd6();
14492 
14493  // Add modifications due to small variations of the SM parameters
14494  mu += cHSM * ( +3.759 * deltaMz()
14495  -0.343 * deltaaMZ()
14496  +2.459 * deltaGmu() );
14497 
14498  } else if (Pol_em == -80. && Pol_ep == 0.){
14499  mu +=
14500  -29686. * CiHL1_11 / LambdaNP2
14501  -1698.32 * CiHe_11 / LambdaNP2
14502  +271004. * CiHL3_11 / LambdaNP2
14503  -84881.5 * CiHD / LambdaNP2
14504  -177249. * CiHWB / LambdaNP2
14505  +1732.98 * CiDHB / LambdaNP2
14506  +4380.98 * CiDHW / LambdaNP2
14507  +7742.96 * CiW / LambdaNP2
14508  -2.828 * DeltaGF()
14509  -0.915 * deltaMwd6();
14510 
14511  // Add modifications due to small variations of the SM parameters
14512  mu += cHSM * ( +4.244 * deltaMz()
14513  -0.624 * deltaaMZ()
14514  +2.729 * deltaGmu() );
14515 
14516  } else {
14517  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14518  }
14519 
14520  } else if (sqrt_s == 0.350) {
14521 
14522  if (Pol_em == 80. && Pol_ep == -30.){
14523  mu +=
14524  -43312.4 * CiHL1_11 / LambdaNP2
14525  -370403. * CiHe_11 / LambdaNP2
14526  +262809. * CiHL3_11 / LambdaNP2
14527  -76119.5 * CiHD / LambdaNP2
14528  -35565.5 * CiHWB / LambdaNP2
14529  +48488.8 * CiDHB / LambdaNP2
14530  -4519.05 * CiDHW / LambdaNP2
14531  +6279.71 * CiW / LambdaNP2
14532  -2.571 * DeltaGF()
14533  -1.059 * deltaMwd6();
14534 
14535  // Add modifications due to small variations of the SM parameters
14536  mu += cHSM * ( +4.035 * deltaMz()
14537  -0.336 * deltaaMZ()
14538  +2.471 * deltaGmu() );
14539 
14540  } else if (Pol_em == -80. && Pol_ep == 30.){
14541  mu +=
14542  -47925. * CiHL1_11 / LambdaNP2
14543  -912.302 * CiHe_11 / LambdaNP2
14544  +290384. * CiHL3_11 / LambdaNP2
14545  -84475.3 * CiHD / LambdaNP2
14546  -177142. * CiHWB / LambdaNP2
14547  +3105.71 * CiDHB / LambdaNP2
14548  +7205.25 * CiDHW / LambdaNP2
14549  +10660.4 * CiW / LambdaNP2
14550  -2.841 * DeltaGF()
14551  -0.773 * deltaMwd6();
14552 
14553  // Add modifications due to small variations of the SM parameters
14554  mu += cHSM * ( +4.542 * deltaMz()
14555  -0.672 * deltaaMZ()
14556  +2.797 * deltaGmu() );
14557 
14558  } else if (Pol_em == 80. && Pol_ep == 0.){
14559  mu +=
14560  -45448.7 * CiHL1_11 / LambdaNP2
14561  -208484. * CiHe_11 / LambdaNP2
14562  +274583. * CiHL3_11 / LambdaNP2
14563  -80024.1 * CiHD / LambdaNP2
14564  -97902.7 * CiHWB / LambdaNP2
14565  +28562.8 * CiDHB / LambdaNP2
14566  +575.898 * CiDHW / LambdaNP2
14567  +8122.74 * CiW / LambdaNP2
14568  -2.687 * DeltaGF()
14569  -0.928 * deltaMwd6();
14570 
14571  // Add modifications due to small variations of the SM parameters
14572  mu += cHSM * ( +4.257 * deltaMz()
14573  -0.496 * deltaaMZ()
14574  +2.607 * deltaGmu() );
14575 
14576  } else if (Pol_em == -80. && Pol_ep == 0.){
14577  mu +=
14578  -47903.7 * CiHL1_11 / LambdaNP2
14579  -2144.19 * CiHe_11 / LambdaNP2
14580  +290349. * CiHL3_11 / LambdaNP2
14581  -84405.4 * CiHD / LambdaNP2
14582  -176530. * CiHWB / LambdaNP2
14583  +3309.62 * CiDHB / LambdaNP2
14584  +7174.21 * CiDHW / LambdaNP2
14585  +10675.5 * CiW / LambdaNP2
14586  -2.84 * DeltaGF()
14587  -0.777 * deltaMwd6();
14588 
14589  // Add modifications due to small variations of the SM parameters
14590  mu += cHSM * ( +4.543 * deltaMz()
14591  -0.674 * deltaaMZ()
14592  +2.798 * deltaGmu() );
14593 
14594  } else {
14595  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14596  }
14597 
14598  } else if (sqrt_s == 0.365) {
14599 
14600  if (Pol_em == 80. && Pol_ep == -30.){
14601  mu +=
14602  -45618.2 * CiHL1_11 / LambdaNP2
14603  -382668. * CiHe_11 / LambdaNP2
14604  +265703. * CiHL3_11 / LambdaNP2
14605  -77085.4 * CiHD / LambdaNP2
14606  -38791. * CiHWB / LambdaNP2
14607  +51079.9 * CiDHB / LambdaNP2
14608  -3972.2 * CiDHW / LambdaNP2
14609  +6727.91 * CiW / LambdaNP2
14610  -2.582 * DeltaGF()
14611  -1.04 * deltaMwd6();
14612 
14613  // Add modifications due to small variations of the SM parameters
14614  mu += cHSM * ( +4.09 * deltaMz()
14615  -0.349 * deltaaMZ()
14616  +2.483 * deltaGmu() );
14617 
14618  } else if (Pol_em == -80. && Pol_ep == 30.){
14619  mu +=
14620  -50230.7 * CiHL1_11 / LambdaNP2
14621  -1000.53 * CiHe_11 / LambdaNP2
14622  +291951. * CiHL3_11 / LambdaNP2
14623  -84657.2 * CiHD / LambdaNP2
14624  -177196. * CiHWB / LambdaNP2
14625  +3348.72 * CiDHB / LambdaNP2
14626  +7579.53 * CiDHW / LambdaNP2
14627  +10879.2 * CiW / LambdaNP2
14628  -2.84 * DeltaGF()
14629  -0.753 * deltaMwd6();
14630 
14631  // Add modifications due to small variations of the SM parameters
14632  mu += cHSM * ( +4.576 * deltaMz()
14633  -0.681 * deltaaMZ()
14634  +2.795 * deltaGmu() );
14635 
14636  } else {
14637  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14638  }
14639 
14640  } else if (sqrt_s == 0.380) {
14641 
14642  if (Pol_em == 80. && Pol_ep == 0.){
14643  mu +=
14644  -49806.5 * CiHL1_11 / LambdaNP2
14645  -221155. * CiHe_11 / LambdaNP2
14646  +280445. * CiHL3_11 / LambdaNP2
14647  -80550.4 * CiHD / LambdaNP2
14648  -101476. * CiHWB / LambdaNP2
14649  +31723.3 * CiDHB / LambdaNP2
14650  +1672.16 * CiDHW / LambdaNP2
14651  +8838.57 * CiW / LambdaNP2
14652  -2.707 * DeltaGF()
14653  -0.891 * deltaMwd6();
14654 
14655  // Add modifications due to small variations of the SM parameters
14656  mu += cHSM * ( +4.331 * deltaMz()
14657  -0.503 * deltaaMZ()
14658  +2.64 * deltaGmu() );
14659 
14660  } else if (Pol_em == -80. && Pol_ep == 0.){
14661  mu +=
14662  -52386.5 * CiHL1_11 / LambdaNP2
14663  -2537.08 * CiHe_11 / LambdaNP2
14664  +294134. * CiHL3_11 / LambdaNP2
14665  -84922.5 * CiHD / LambdaNP2
14666  -176871. * CiHWB / LambdaNP2
14667  +3635.55 * CiDHB / LambdaNP2
14668  +7973.68 * CiDHW / LambdaNP2
14669  +10984.7 * CiW / LambdaNP2
14670  -2.838 * DeltaGF()
14671  -0.753 * deltaMwd6();
14672 
14673  // Add modifications due to small variations of the SM parameters
14674  mu += cHSM * ( +4.589 * deltaMz()
14675  -0.68 * deltaaMZ()
14676  +2.81 * deltaGmu() );
14677 
14678  } else {
14679  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14680  }
14681 
14682  } else if (sqrt_s == 0.500) {
14683 
14684  if (Pol_em == 80. && Pol_ep == -30.){
14685  mu +=
14686  -64264.6 * CiHL1_11 / LambdaNP2
14687  -495727. * CiHe_11 / LambdaNP2
14688  +289682. * CiHL3_11 / LambdaNP2
14689  -80108.8 * CiHD / LambdaNP2
14690  -61678. * CiHWB / LambdaNP2
14691  +75403.3 * CiDHB / LambdaNP2
14692  +458.146 * CiDHW / LambdaNP2
14693  +8723.87 * CiW / LambdaNP2
14694  -2.664 * DeltaGF()
14695  -0.849 * deltaMwd6();
14696 
14697  // Add modifications due to small variations of the SM parameters
14698  mu += cHSM * ( +4.362 * deltaMz()
14699  -0.496 * deltaaMZ()
14700  +2.591 * deltaGmu() );
14701 
14702  } else if (Pol_em == -80. && Pol_ep == 30.){
14703  mu +=
14704  -68310.7 * CiHL1_11 / LambdaNP2
14705  -1341.22 * CiHe_11 / LambdaNP2
14706  +311528. * CiHL3_11 / LambdaNP2
14707  -84984.5 * CiHD / LambdaNP2
14708  -178260. * CiHWB / LambdaNP2
14709  +5206.37 * CiDHB / LambdaNP2
14710  +10705.4 * CiDHW / LambdaNP2
14711  +11071.1 * CiW / LambdaNP2
14712  -2.855 * DeltaGF()
14713  -0.671 * deltaMwd6();
14714 
14715  // Add modifications due to small variations of the SM parameters
14716  mu += cHSM * ( +4.728 * deltaMz()
14717  -0.698 * deltaaMZ()
14718  +2.817 * deltaGmu() );
14719 
14720  } else if (Pol_em == 80. && Pol_ep == 0.){
14721  mu +=
14722  -66178. * CiHL1_11 / LambdaNP2
14723  -274919. * CiHe_11 / LambdaNP2
14724  +299745. * CiHL3_11 / LambdaNP2
14725  -82524.6 * CiHD / LambdaNP2
14726  -113979. * CiHWB / LambdaNP2
14727  +43898.4 * CiDHB / LambdaNP2
14728  +5024.43 * CiDHW / LambdaNP2
14729  +9759.79 * CiW / LambdaNP2
14730  -2.752 * DeltaGF()
14731  -0.778 * deltaMwd6();
14732 
14733  // Add modifications due to small variations of the SM parameters
14734  mu += cHSM * ( +4.515 * deltaMz()
14735  -0.602 * deltaaMZ()
14736  +2.695 * deltaGmu() );
14737 
14738  } else if (Pol_em == -80. && Pol_ep == 0.){
14739  mu +=
14740  -68435.6 * CiHL1_11 / LambdaNP2
14741  -3089.11 * CiHe_11 / LambdaNP2
14742  +310020. * CiHL3_11 / LambdaNP2
14743  -85227.7 * CiHD / LambdaNP2
14744  -178139. * CiHWB / LambdaNP2
14745  +5322.77 * CiDHB / LambdaNP2
14746  +10598. * CiDHW / LambdaNP2
14747  +11009.9 * CiW / LambdaNP2
14748  -2.846 * DeltaGF()
14749  -0.681 * deltaMwd6();
14750 
14751  // Add modifications due to small variations of the SM parameters
14752  mu += cHSM * ( +4.725 * deltaMz()
14753  -0.695 * deltaaMZ()
14754  +2.828 * deltaGmu() );
14755 
14756  } else {
14757  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14758  }
14759 
14760  } else if (sqrt_s == 1.0) {
14761 
14762  if (Pol_em == 80. && Pol_ep == -20.){
14763  mu +=
14764  -145951. * CiHL1_11 / LambdaNP2
14765  -885593. * CiHe_11 / LambdaNP2
14766  +383080. * CiHL3_11 / LambdaNP2
14767  -83628.6 * CiHD / LambdaNP2
14768  -114732. * CiHWB / LambdaNP2
14769  +159832. * CiDHB / LambdaNP2
14770  +17735.5 * CiDHW / LambdaNP2
14771  +8916.37 * CiW / LambdaNP2
14772  -2.787 * DeltaGF()
14773  -0.57 * deltaMwd6() ;
14774 
14775  // Add modifications due to small variations of the SM parameters
14776  mu += cHSM * ( +4.793 * deltaMz()
14777  -0.653 * deltaaMZ()
14778  +2.677 * deltaGmu() );
14779 
14780  } else if (Pol_em == -80. && Pol_ep == 20.){
14781  mu +=
14782  -150086. * CiHL1_11 / LambdaNP2
14783  -4395.1 * CiHe_11 / LambdaNP2
14784  +394641. * CiHL3_11 / LambdaNP2
14785  -85925.1 * CiHD / LambdaNP2
14786  -181046. * CiHWB / LambdaNP2
14787  +13333.6 * CiDHB / LambdaNP2
14788  +23871.2 * CiDHW / LambdaNP2
14789  +9450.35 * CiW / LambdaNP2
14790  -2.871 * DeltaGF()
14791  -0.492 * deltaMwd6() ;
14792 
14793  // Add modifications due to small variations of the SM parameters
14794  mu += cHSM * ( +5.001 * deltaMz()
14795  -0.752 * deltaaMZ()
14796  +2.79 * deltaGmu() );
14797 
14798  } else {
14799  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14800  }
14801 
14802  } else if (sqrt_s == 1.5) {
14803 
14804  if (Pol_em == 80. && Pol_ep == 0.){
14805  mu +=
14806  -261040. * CiHL1_11 / LambdaNP2
14807  -1059495. * CiHe_11 / LambdaNP2
14808  +500666. * CiHL3_11 / LambdaNP2
14809  -84992.3 * CiHD / LambdaNP2
14810  -144925. * CiHWB / LambdaNP2
14811  +205215. * CiDHB / LambdaNP2
14812  +38777.5 * CiDHW / LambdaNP2
14813  +7857.84 * CiW / LambdaNP2
14814  -2.817 * DeltaGF()
14815  -0.471 * deltaMwd6();
14816 
14817  // Add modifications due to small variations of the SM parameters
14818  mu += cHSM * ( +4.975 * deltaMz()
14819  -0.718 * deltaaMZ()
14820  +2.688 * deltaGmu() );
14821 
14822  } else if (Pol_em == -80. && Pol_ep == 0.){
14823  mu +=
14824  -265008. * CiHL1_11 / LambdaNP2
14825  -13002.4 * CiHe_11 / LambdaNP2
14826  +507924. * CiHL3_11 / LambdaNP2
14827  -86313.9 * CiHD / LambdaNP2
14828  -182113. * CiHWB / LambdaNP2
14829  +24953.6 * CiDHB / LambdaNP2
14830  +42429.8 * CiDHW / LambdaNP2
14831  +8014.86 * CiW / LambdaNP2
14832  -2.857 * DeltaGF()
14833  -0.429 * deltaMwd6();
14834 
14835  // Add modifications due to small variations of the SM parameters
14836  mu += cHSM * ( +5.094 * deltaMz()
14837  -0.768 * deltaaMZ()
14838  +2.739 * deltaGmu() );
14839 
14840  } else {
14841  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14842  }
14843 
14844  } else if (sqrt_s == 3.0) {
14845 
14846  if (Pol_em == 80. && Pol_ep == 0.){
14847  mu +=
14848  -776767. * CiHL1_11 / LambdaNP2
14849  -3168410. * CiHe_11 / LambdaNP2
14850  +1016120. * CiHL3_11 / LambdaNP2
14851  -85414.3 * CiHD / LambdaNP2
14852  -155729. * CiHWB / LambdaNP2
14853  +628130. * CiDHB / LambdaNP2
14854  +123368. * CiDHW / LambdaNP2
14855  +6454.34 * CiW / LambdaNP2
14856  -2.831 * DeltaGF()
14857  -0.352 * deltaMwd6();
14858 
14859  // Add modifications due to small variations of the SM parameters
14860  mu += cHSM * ( +5.165 * deltaMz()
14861  -0.755 * deltaaMZ()
14862  +2.77 * deltaGmu() );
14863 
14864  } else if (Pol_em == -80. && Pol_ep == 0.){
14865  mu +=
14866  -785359. * CiHL1_11 / LambdaNP2
14867  -39533. * CiHe_11 / LambdaNP2
14868  +1027322. * CiHL3_11 / LambdaNP2
14869  -86621.7 * CiHD / LambdaNP2
14870  -184516. * CiHWB / LambdaNP2
14871  +75975.5 * CiDHB / LambdaNP2
14872  +127086. * CiDHW / LambdaNP2
14873  +6519.78 * CiW / LambdaNP2
14874  -2.86 * DeltaGF()
14875  -0.328 * deltaMwd6();
14876 
14877  // Add modifications due to small variations of the SM parameters
14878  mu += cHSM * ( +5.246 * deltaMz()
14879  -0.79 * deltaaMZ()
14880  +2.81 * deltaGmu() );
14881 
14882  } else {
14883  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14884  }
14885 
14886  } else
14887  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeWWPol()");
14888 
14889  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
14890 
14891  return mu;
14892 }

◆ mueeZBF()

double NPSMEFTd6::mueeZBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZBF}\)

Reimplemented from NPbase.

Definition at line 5683 of file NPSMEFTd6.cpp.

5684 {
5685  double mu = 1.0;
5686 
5687  double C1 = 0.0;
5688 
5689  if (sqrt_s == 0.240) {
5690 
5691  C1 = 0.0070;
5692 
5693  mu +=
5694  +121661. * CiHbox / LambdaNP2
5695  +489617. * CiHL1_11 / LambdaNP2
5696  -357163. * CiHe_11 / LambdaNP2
5697  +489617. * CiHL3_11 / LambdaNP2
5698  -39217.8 * CiHD / LambdaNP2
5699  +1525468. * CiHB / LambdaNP2
5700  +378019. * CiHW / LambdaNP2
5701  +215983. * CiHWB / LambdaNP2
5702  -6554.11 * CiDHB / LambdaNP2
5703  +1175.47 * CiDHW / LambdaNP2
5704  -3.161 * DeltaGF()
5705  ;
5706 
5707  // Add modifications due to small variations of the SM parameters
5708  mu += cHSM * ( +0.908 * deltaMz()
5709  -5.799 * deltaMh()
5710  -0.248 * deltaaMZ()
5711  +3.158 * deltaGmu() );
5712 
5713  if (FlagQuadraticTerms) {
5714  //Add contributions that are quadratic in the effective coefficients
5715  mu += 0.0;
5716  }
5717 
5718  } else if (sqrt_s == 0.250) {
5719 
5720  C1 = 0.0070;
5721 
5722  mu +=
5723  +122144. * CiHbox / LambdaNP2
5724  +444406. * CiHL1_11 / LambdaNP2
5725  -315727. * CiHe_11 / LambdaNP2
5726  +444406. * CiHL3_11 / LambdaNP2
5727  -41440.8 * CiHD / LambdaNP2
5728  +1186855. * CiHB / LambdaNP2
5729  +301913. * CiHW / LambdaNP2
5730  +98540.5 * CiHWB / LambdaNP2
5731  -5766.35 * CiDHB / LambdaNP2
5732  +294.724 * CiDHW / LambdaNP2
5733  -3.279 * DeltaGF()
5734  ;
5735 
5736  // Add modifications due to small variations of the SM parameters
5737  mu += cHSM * ( +2.044 * deltaMz()
5738  -4.578 * deltaMh()
5739  -0.341 * deltaaMZ()
5740  +3.283 * deltaGmu() );
5741 
5742  if (FlagQuadraticTerms) {
5743  //Add contributions that are quadratic in the effective coefficients
5744  mu += 0.0;
5745  }
5746 
5747  } else if (sqrt_s == 0.350) {
5748 
5749  C1 = 0.0069;
5750 
5751  mu +=
5752  +121556. * CiHbox / LambdaNP2
5753  +46354.9 * CiHL1_11 / LambdaNP2
5754  -251.929 * CiHe_11 / LambdaNP2
5755  +46354.9 * CiHL3_11 / LambdaNP2
5756  -43426.2 * CiHD / LambdaNP2
5757  +450512. * CiHB / LambdaNP2
5758  +166493. * CiHW / LambdaNP2
5759  -198898. * CiHWB / LambdaNP2
5760  -4408.76 * CiDHB / LambdaNP2
5761  -17005.2 * CiDHW / LambdaNP2
5762  -3.427 * DeltaGF()
5763  ;
5764 
5765  // Add modifications due to small variations of the SM parameters
5766  mu += cHSM * ( +3.845 * deltaMz()
5767  -1.857 * deltaMh()
5768  -0.423 * deltaaMZ()
5769  +3.407 * deltaGmu() );
5770 
5771  if (FlagQuadraticTerms) {
5772  //Add contributions that are quadratic in the effective coefficients
5773  mu += 0.0;
5774  }
5775 
5776  } else if (sqrt_s == 0.365) {
5777 
5778  C1 = 0.0069; // use same as 350 GeV
5779 
5780  mu +=
5781  +121067. * CiHbox / LambdaNP2
5782  +9887.64 * CiHL1_11 / LambdaNP2
5783  +27809. * CiHe_11 / LambdaNP2
5784  +9887.64 * CiHL3_11 / LambdaNP2
5785  -43174.2 * CiHD / LambdaNP2
5786  +417865. * CiHB / LambdaNP2
5787  +154270. * CiHW / LambdaNP2
5788  -201517. * CiHWB / LambdaNP2
5789  -4943.82 * CiDHB / LambdaNP2
5790  -19213.5 * CiDHW / LambdaNP2
5791  -3.423 * DeltaGF()
5792  ;
5793 
5794  // Add modifications due to small variations of the SM parameters
5795  mu += cHSM * ( +3.861 * deltaMz()
5796  -1.736 * deltaMh()
5797  -0.426 * deltaaMZ()
5798  +3.375 * deltaGmu() );
5799 
5800  if (FlagQuadraticTerms) {
5801  //Add contributions that are quadratic in the effective coefficients
5802  mu += 0.0;
5803  }
5804 
5805  } else if (sqrt_s == 0.380) {
5806 
5807  C1 = 0.0069; // use same as 350 GeV
5808 
5809  mu +=
5810  +121214. * CiHbox / LambdaNP2
5811  -22289.7 * CiHL1_11 / LambdaNP2
5812  +52903.2 * CiHe_11 / LambdaNP2
5813  -22289.7 * CiHL3_11 / LambdaNP2
5814  -43137.3 * CiHD / LambdaNP2
5815  +388336. * CiHB / LambdaNP2
5816  +140923. * CiHW / LambdaNP2
5817  -202884. * CiHWB / LambdaNP2
5818  -5363.69 * CiDHB / LambdaNP2
5819  -21404.2 * CiDHW / LambdaNP2
5820  -3.418 * DeltaGF()
5821  ;
5822 
5823  // Add modifications due to small variations of the SM parameters
5824  mu += cHSM * ( +3.887 * deltaMz()
5825  -1.633 * deltaMh()
5826  -0.419 * deltaaMZ()
5827  +3.393 * deltaGmu() );
5828 
5829  if (FlagQuadraticTerms) {
5830  //Add contributions that are quadratic in the effective coefficients
5831  mu += 0.0;
5832  }
5833 
5834  } else if (sqrt_s == 0.500) {
5835 
5836  C1 = 0.0067;
5837 
5838  mu +=
5839  +121453. * CiHbox / LambdaNP2
5840  -185326. * CiHL1_11 / LambdaNP2
5841  +178925. * CiHe_11 / LambdaNP2
5842  -185326. * CiHL3_11 / LambdaNP2
5843  -42051.6 * CiHD / LambdaNP2
5844  +236945. * CiHB / LambdaNP2
5845  +67833.5 * CiHW / LambdaNP2
5846  -178623. * CiHWB / LambdaNP2
5847  -8004.61 * CiDHB / LambdaNP2
5848  -33567.3 * CiDHW / LambdaNP2
5849  -3.416 * DeltaGF()
5850  ;
5851 
5852  // Add modifications due to small variations of the SM parameters
5853  mu += cHSM * ( +3.963 * deltaMz()
5854  -1.143 * deltaMh()
5855  -0.408 * deltaaMZ()
5856  +3.383 * deltaGmu() );
5857 
5858  if (FlagQuadraticTerms) {
5859  //Add contributions that are quadratic in the effective coefficients
5860  mu += 0.0;
5861  }
5862 
5863  } else if (sqrt_s == 1.0) {
5864 
5865  C1 = 0.0065;
5866 
5867  mu +=
5868  +121062. * CiHbox / LambdaNP2
5869  -409543. * CiHL1_11 / LambdaNP2
5870  +356730. * CiHe_11 / LambdaNP2
5871  -409543. * CiHL3_11 / LambdaNP2
5872  -42133.9 * CiHD / LambdaNP2
5873  +69851. * CiHB / LambdaNP2
5874  -14416.8 * CiHW / LambdaNP2
5875  -113198. * CiHWB / LambdaNP2
5876  -18688.4 * CiDHB / LambdaNP2
5877  -61696. * CiDHW / LambdaNP2
5878  -3.405 * DeltaGF()
5879  ;
5880 
5881  // Add modifications due to small variations of the SM parameters
5882  mu += cHSM * ( +4.216 * deltaMz()
5883  -0.546 * deltaMh()
5884  -0.407 * deltaaMZ()
5885  +3.393 * deltaGmu() );
5886 
5887  if (FlagQuadraticTerms) {
5888  //Add contributions that are quadratic in the effective coefficients
5889  mu += 0.0;
5890  }
5891 
5892  } else if (sqrt_s == 1.4) {
5893 
5894  C1 = 0.0065;
5895 
5896  mu +=
5897  +120749. * CiHbox / LambdaNP2
5898  -493617. * CiHL1_11 / LambdaNP2
5899  +426669. * CiHe_11 / LambdaNP2
5900  -493617. * CiHL3_11 / LambdaNP2
5901  -42486.9 * CiHD / LambdaNP2
5902  +34633.1 * CiHB / LambdaNP2
5903  -27609.6 * CiHW / LambdaNP2
5904  -97014.2 * CiHWB / LambdaNP2
5905  -23942.2 * CiDHB / LambdaNP2
5906  -74940.3 * CiDHW / LambdaNP2
5907  -3.405 * DeltaGF()
5908  ;
5909 
5910  // Add modifications due to small variations of the SM parameters
5911  mu += cHSM * ( +4.309 * deltaMz()
5912  -0.422 * deltaMh()
5913  -0.402 * deltaaMZ()
5914  +3.379 * deltaGmu() );
5915 
5916  if (FlagQuadraticTerms) {
5917  //Add contributions that are quadratic in the effective coefficients
5918  mu += 0.0;
5919  }
5920 
5921  } else if (sqrt_s == 1.5) {
5922 
5923  C1 = 0.0065;// Use the same as 1400 GeV
5924 
5925  mu +=
5926  +120587. * CiHbox / LambdaNP2
5927  -510290. * CiHL1_11 / LambdaNP2
5928  +440504. * CiHe_11 / LambdaNP2
5929  -510290. * CiHL3_11 / LambdaNP2
5930  -42529.6 * CiHD / LambdaNP2
5931  +30448.1 * CiHB / LambdaNP2
5932  -30741.2 * CiHW / LambdaNP2
5933  -95903.3 * CiHWB / LambdaNP2
5934  -25074.9 * CiDHB / LambdaNP2
5935  -77634.5 * CiDHW / LambdaNP2
5936  -3.401 * DeltaGF()
5937  ;
5938 
5939  // Add modifications due to small variations of the SM parameters
5940  mu += cHSM * ( +4.326 * deltaMz()
5941  -0.4 * deltaMh()
5942  -0.403 * deltaaMZ()
5943  +3.37 * deltaGmu() );
5944 
5945  if (FlagQuadraticTerms) {
5946  //Add contributions that are quadratic in the effective coefficients
5947  mu += 0.0;
5948  }
5949 
5950  } else if (sqrt_s == 3.0) {
5951 
5952  C1 = 0.0063;
5953 
5954  mu +=
5955  +120474. * CiHbox / LambdaNP2
5956  -677185. * CiHL1_11 / LambdaNP2
5957  +582037. * CiHe_11 / LambdaNP2
5958  -677185. * CiHL3_11 / LambdaNP2
5959  -42541.3 * CiHD / LambdaNP2
5960  +6810.6 * CiHB / LambdaNP2
5961  -32994.5 * CiHW / LambdaNP2
5962  -78012.3 * CiHWB / LambdaNP2
5963  -36250. * CiDHB / LambdaNP2
5964  -105734. * CiDHW / LambdaNP2
5965  -3.405 * DeltaGF()
5966  ;
5967 
5968  // Add modifications due to small variations of the SM parameters
5969  mu += cHSM * ( +4.463 * deltaMz()
5970  -0.265 * deltaMh()
5971  -0.405 * deltaaMZ()
5972  +3.351 * deltaGmu() );
5973 
5974  if (FlagQuadraticTerms) {
5975  //Add contributions that are quadratic in the effective coefficients
5976  mu += 0.0;
5977  }
5978 
5979  } else
5980  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBF()");
5981 
5982  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
5983  //(Assume similar to WBF.)
5984  mu += eeeWBFint + eeeWBFpar;
5985 
5986 // Linear contribution from Higgs self-coupling
5987  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
5988 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
5990 
5991  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
5992 
5993  return mu;
5994 }

◆ mueeZBFPol()

double NPSMEFTd6::mueeZBFPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZBF}\)

Reimplemented from NPbase.

Definition at line 5997 of file NPSMEFTd6.cpp.

5998 {
5999  double mu = 1.0;
6000 
6001  double C1 = 0.0;
6002 
6003  if (sqrt_s == 0.240) {
6004 
6005  C1 = 0.0070;
6006 
6007  if (Pol_em == 80. && Pol_ep == -30.){
6008  mu +=
6009  +121531. * CiHbox / LambdaNP2
6010  +58943.5 * CiHL1_11 / LambdaNP2
6011  -939512. * CiHe_11 / LambdaNP2
6012  +58943.5 * CiHL3_11 / LambdaNP2
6013  +77442.6 * CiHD / LambdaNP2
6014  +2082256. * CiHB / LambdaNP2
6015  +108043. * CiHW / LambdaNP2
6016  +1362693. * CiHWB / LambdaNP2
6017  +40385. * CiDHB / LambdaNP2
6018  -21886. * CiDHW / LambdaNP2
6019  +0.563 * DeltaGF()
6020  ;
6021 
6022  // Add modifications due to small variations of the SM parameters
6023  mu += cHSM * ( -6.582 * deltaMz()
6024  -5.732 * deltaMh()
6025  +3.573 * deltaaMZ()
6026  -0.708 * deltaGmu() );
6027 
6028  } else if (Pol_em == -80. && Pol_ep == 30.){
6029  mu +=
6030  +122065. * CiHbox / LambdaNP2
6031  +905327. * CiHL1_11 / LambdaNP2
6032  -55689. * CiHe_11 / LambdaNP2
6033  +905327. * CiHL3_11 / LambdaNP2
6034  -124548. * CiHD / LambdaNP2
6035  +905057. * CiHB / LambdaNP2
6036  +540185. * CiHW / LambdaNP2
6037  -329708. * CiHWB / LambdaNP2
6038  -37296.9 * CiDHB / LambdaNP2
6039  +20497.1 * CiDHW / LambdaNP2
6040  -5.854 * DeltaGF()
6041  ;
6042 
6043  // Add modifications due to small variations of the SM parameters
6044  mu += cHSM * ( +6.473 * deltaMz()
6045  -5.971 * deltaMh()
6046  -3.019 * deltaaMZ()
6047  +5.959 * deltaGmu() );
6048 
6049  } else if (Pol_em == 80. && Pol_ep == 0.){
6050  mu +=
6051  +121947. * CiHbox / LambdaNP2
6052  +88774.4 * CiHL1_11 / LambdaNP2
6053  -753269. * CiHe_11 / LambdaNP2
6054  +88774.4 * CiHL3_11 / LambdaNP2
6055  +54593.2 * CiHD / LambdaNP2
6056  +2101955. * CiHB / LambdaNP2
6057  +182237. * CiHW / LambdaNP2
6058  +972861. * CiHWB / LambdaNP2
6059  +29346.2 * CiDHB / LambdaNP2
6060  -18562.1 * CiDHW / LambdaNP2
6061  -0.206 * DeltaGF()
6062  ;
6063 
6064  // Add modifications due to small variations of the SM parameters
6065  mu += cHSM * ( -5.131 * deltaMz()
6066  -5.658 * deltaMh()
6067  +2.794 * deltaaMZ()
6068  +0.082 * deltaGmu() );
6069 
6070  } else if (Pol_em == -80. && Pol_ep == 0.){
6071  mu +=
6072  +122265. * CiHbox / LambdaNP2
6073  +785643. * CiHL1_11 / LambdaNP2
6074  -66907.6 * CiHe_11 / LambdaNP2
6075  +785643. * CiHL3_11 / LambdaNP2
6076  -107673. * CiHD / LambdaNP2
6077  +1115316. * CiHB / LambdaNP2
6078  +521873. * CiHW / LambdaNP2
6079  -331727. * CiHWB / LambdaNP2
6080  -32442.4 * CiDHB / LambdaNP2
6081  +15348.7 * CiDHW / LambdaNP2
6082  -5.334 * DeltaGF()
6083  ;
6084 
6085  // Add modifications due to small variations of the SM parameters
6086  mu += cHSM * ( +5.367 * deltaMz()
6087  -5.87 * deltaMh()
6088  -2.491 * deltaaMZ()
6089  +5.409 * deltaGmu() );
6090 
6091  } else {
6092  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6093  }
6094 
6095  } else if (sqrt_s == 0.250) {
6096 
6097  C1 = 0.0070;
6098 
6099  if (Pol_em == 80. && Pol_ep == -30.){
6100  mu +=
6101  +121054. * CiHbox / LambdaNP2
6102  +51113. * CiHL1_11 / LambdaNP2
6103  -851357. * CiHe_11 / LambdaNP2
6104  +51113. * CiHL3_11 / LambdaNP2
6105  +76762.9 * CiHD / LambdaNP2
6106  +1629614. * CiHB / LambdaNP2
6107  +72741.6 * CiHW / LambdaNP2
6108  +1130834. * CiHWB / LambdaNP2
6109  +34381.7 * CiDHB / LambdaNP2
6110  -19876.5 * CiDHW / LambdaNP2
6111  +0.563 * DeltaGF()
6112  ;
6113 
6114  // Add modifications due to small variations of the SM parameters
6115  mu += cHSM * ( -5.658 * deltaMz()
6116  -4.485 * deltaMh()
6117  +3.577 * deltaaMZ()
6118  -0.638 * deltaGmu() );
6119 
6120  } else if (Pol_em == -80. && Pol_ep == 30.){
6121  mu +=
6122  +121471. * CiHbox / LambdaNP2
6123  +824294. * CiHL1_11 / LambdaNP2
6124  -45066.5 * CiHe_11 / LambdaNP2
6125  +824294. * CiHL3_11 / LambdaNP2
6126  -128864. * CiHD / LambdaNP2
6127  +644513. * CiHB / LambdaNP2
6128  +425051. * CiHW / LambdaNP2
6129  -383720. * CiHWB / LambdaNP2
6130  -32434.3 * CiDHB / LambdaNP2
6131  +15329.4 * CiDHW / LambdaNP2
6132  -6.022 * DeltaGF()
6133  ;
6134 
6135  // Add modifications due to small variations of the SM parameters
6136  mu += cHSM * ( +7.852 * deltaMz()
6137  -4.536 * deltaMh()
6138  -3.165 * deltaaMZ()
6139  +6.136 * deltaGmu() );
6140 
6141  } else if (Pol_em == 80. && Pol_ep == 0.){
6142  mu +=
6143  +121494. * CiHbox / LambdaNP2
6144  +77372.1 * CiHL1_11 / LambdaNP2
6145  -676199. * CiHe_11 / LambdaNP2
6146  +77372.1 * CiHL3_11 / LambdaNP2
6147  +53294.7 * CiHD / LambdaNP2
6148  +1668830. * CiHB / LambdaNP2
6149  +145010. * CiHW / LambdaNP2
6150  +772902. * CiHWB / LambdaNP2
6151  +23910.6 * CiDHB / LambdaNP2
6152  -16890.6 * CiDHW / LambdaNP2
6153  -0.226 * DeltaGF()
6154  ;
6155 
6156  // Add modifications due to small variations of the SM parameters
6157  mu += cHSM * ( -4.183 * deltaMz()
6158  -4.557 * deltaMh()
6159  +2.773 * deltaaMZ()
6160  +0.148 * deltaGmu() );
6161 
6162  } else if (Pol_em == -80. && Pol_ep == 0.){
6163  mu +=
6164  +121947. * CiHbox / LambdaNP2
6165  +713174. * CiHL1_11 / LambdaNP2
6166  -53393.3 * CiHe_11 / LambdaNP2
6167  +713174. * CiHL3_11 / LambdaNP2
6168  -111120. * CiHD / LambdaNP2
6169  +843388. * CiHB / LambdaNP2
6170  +417838. * CiHW / LambdaNP2
6171  -386753. * CiHWB / LambdaNP2
6172  -27915.7 * CiDHB / LambdaNP2
6173  +11946.5 * CiDHW / LambdaNP2
6174  -5.496 * DeltaGF()
6175  ;
6176 
6177  // Add modifications due to small variations of the SM parameters
6178  mu += cHSM * ( +6.641 * deltaMz()
6179  -4.576 * deltaMh()
6180  -2.605 * deltaaMZ()
6181  +5.56 * deltaGmu() );
6182 
6183  } else {
6184  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6185  }
6186 
6187  } else if (sqrt_s == 0.350) {
6188 
6189  C1 = 0.0069;
6190 
6191  if (Pol_em == 80. && Pol_ep == -30.){
6192  mu +=
6193  +121674. * CiHbox / LambdaNP2
6194  -47420.2 * CiHL1_11 / LambdaNP2
6195  -172088. * CiHe_11 / LambdaNP2
6196  -47420.2 * CiHL3_11 / LambdaNP2
6197  +59728. * CiHD / LambdaNP2
6198  +544205. * CiHB / LambdaNP2
6199  +83604.4 * CiHW / LambdaNP2
6200  +435393. * CiHWB / LambdaNP2
6201  -24800.4 * CiDHB / LambdaNP2
6202  -4583.09 * CiDHW / LambdaNP2
6203  -0.05 * DeltaGF()
6204  ;
6205 
6206  // Add modifications due to small variations of the SM parameters
6207  mu += cHSM * ( -2.905 * deltaMz()
6208  -1.842 * deltaMh()
6209  +2.966 * deltaaMZ()
6210  +0.009 * deltaGmu() );
6211 
6212  } else if (Pol_em == -80. && Pol_ep == 30.){
6213  mu +=
6214  +121541. * CiHbox / LambdaNP2
6215  +197618. * CiHL1_11 / LambdaNP2
6216  +42238.9 * CiHe_11 / LambdaNP2
6217  +197618. * CiHL3_11 / LambdaNP2
6218  -124376. * CiHD / LambdaNP2
6219  +181154. * CiHB / LambdaNP2
6220  +195329. * CiHW / LambdaNP2
6221  -505800. * CiHWB / LambdaNP2
6222  +13082.6 * CiDHB / LambdaNP2
6223  -26607.4 * CiDHW / LambdaNP2
6224  -6.096 * DeltaGF()
6225  ;
6226 
6227  // Add modifications due to small variations of the SM parameters
6228  mu += cHSM * ( +9.303 * deltaMz()
6229  -1.82 * deltaMh()
6230  -3.105 * deltaaMZ()
6231  +6.071 * deltaGmu() );
6232 
6233  } else if (Pol_em == 80. && Pol_ep == 0.){
6234  mu +=
6235  +121760. * CiHbox / LambdaNP2
6236  -62853. * CiHL1_11 / LambdaNP2
6237  -83019.6 * CiHe_11 / LambdaNP2
6238  -62853. * CiHL3_11 / LambdaNP2
6239  +34395.4 * CiHD / LambdaNP2
6240  +623389. * CiHB / LambdaNP2
6241  +123932. * CiHW / LambdaNP2
6242  +181789. * CiHWB / LambdaNP2
6243  -20420. * CiDHB / LambdaNP2
6244  -7820.42 * CiDHW / LambdaNP2
6245  -0.875 * DeltaGF()
6246  ;
6247 
6248  // Add modifications due to small variations of the SM parameters
6249  mu += cHSM * ( -1.322 * deltaMz()
6250  -1.873 * deltaMh()
6251  +2.14 * deltaaMZ()
6252  +0.844 * deltaGmu() );
6253 
6254  } else if (Pol_em == -80. && Pol_ep == 0.){
6255  mu +=
6256  +121557. * CiHbox / LambdaNP2
6257  +131443. * CiHL1_11 / LambdaNP2
6258  +63326.7 * CiHe_11 / LambdaNP2
6259  +131443. * CiHL3_11 / LambdaNP2
6260  -103038. * CiHD / LambdaNP2
6261  +323596. * CiHB / LambdaNP2
6262  +201676. * CiHW / LambdaNP2
6263  -491019. * CiHWB / LambdaNP2
6264  +7992.43 * CiDHB / LambdaNP2
6265  -24283.6 * CiDHW / LambdaNP2
6266  -5.391 * DeltaGF()
6267  ;
6268 
6269  // Add modifications due to small variations of the SM parameters
6270  mu += cHSM * ( +7.818 * deltaMz()
6271  -1.846 * deltaMh()
6272  -2.402 * deltaaMZ()
6273  +5.358 * deltaGmu() );
6274 
6275  } else {
6276  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6277  }
6278 
6279  } else if (sqrt_s == 0.365) {
6280 
6281  C1 = 0.0069; // Use same as 350 GeV
6282 
6283  if (Pol_em == 80. && Pol_ep == -30.){
6284  mu +=
6285  +121458. * CiHbox / LambdaNP2
6286  -58695.1 * CiHL1_11 / LambdaNP2
6287  -109686. * CiHe_11 / LambdaNP2
6288  -58695.1 * CiHL3_11 / LambdaNP2
6289  +58496.7 * CiHD / LambdaNP2
6290  +489137. * CiHB / LambdaNP2
6291  +80751.3 * CiHW / LambdaNP2
6292  +410304. * CiHWB / LambdaNP2
6293  -30918.3 * CiDHB / LambdaNP2
6294  -3571.31 * CiDHW / LambdaNP2
6295  -0.085 * DeltaGF()
6296  ;
6297 
6298  // Add modifications due to small variations of the SM parameters
6299  mu += cHSM * ( -2.809 * deltaMz()
6300  -1.721 * deltaMh()
6301  +2.93 * deltaaMZ()
6302  +0.026 * deltaGmu() );
6303 
6304  } else if (Pol_em == -80. && Pol_ep == 30.){
6305  mu +=
6306  +121152. * CiHbox / LambdaNP2
6307  +136019. * CiHL1_11 / LambdaNP2
6308  +50762. * CiHe_11 / LambdaNP2
6309  +136019. * CiHL3_11 / LambdaNP2
6310  -123859. * CiHD / LambdaNP2
6311  +165799. * CiHB / LambdaNP2
6312  +176652. * CiHW / LambdaNP2
6313  -504889. * CiHWB / LambdaNP2
6314  +16920.7 * CiDHB / LambdaNP2
6315  -31414.1 * CiDHW / LambdaNP2
6316  -6.076 * DeltaGF()
6317  ;
6318 
6319  // Add modifications due to small variations of the SM parameters
6320  mu += cHSM * ( +9.271 * deltaMz()
6321  -1.7 * deltaMh()
6322  -3.092 * deltaaMZ()
6323  +6.031 * deltaGmu() );
6324 
6325  } else if (Pol_em == 80. && Pol_ep == 0.){
6326  mu +=
6327  +121193. * CiHbox / LambdaNP2
6328  -76905.7 * CiHL1_11 / LambdaNP2
6329  -32264.3 * CiHe_11 / LambdaNP2
6330  -76905.7 * CiHL3_11 / LambdaNP2
6331  +33650.3 * CiHD / LambdaNP2
6332  +573505. * CiHB / LambdaNP2
6333  +117937. * CiHW / LambdaNP2
6334  +166382. * CiHWB / LambdaNP2
6335  -25012.1 * CiDHB / LambdaNP2
6336  -7703.47 * CiDHW / LambdaNP2
6337  -0.911 * DeltaGF()
6338  ;
6339 
6340  // Add modifications due to small variations of the SM parameters
6341  mu += cHSM * ( -1.233 * deltaMz()
6342  -1.746 * deltaMh()
6343  +2.101 * deltaaMZ()
6344  +0.861 * deltaGmu() );
6345 
6346  } else if (Pol_em == -80. && Pol_ep == 0.){
6347  mu +=
6348  +121177. * CiHbox / LambdaNP2
6349  +77981.5 * CiHL1_11 / LambdaNP2
6350  +74274.1 * CiHe_11 / LambdaNP2
6351  +77981.5 * CiHL3_11 / LambdaNP2
6352  -102068. * CiHD / LambdaNP2
6353  +305730. * CiHB / LambdaNP2
6354  +183682. * CiHW / LambdaNP2
6355  -487770. * CiHWB / LambdaNP2
6356  +10624.8 * CiDHB / LambdaNP2
6357  -28092.3 * CiDHW / LambdaNP2
6358  -5.366 * DeltaGF()
6359  ;
6360 
6361  // Add modifications due to small variations of the SM parameters
6362  mu += cHSM * ( +7.791 * deltaMz()
6363  -1.726 * deltaMh()
6364  -2.377 * deltaaMZ()
6365  +5.325 * deltaGmu() );
6366 
6367  } else {
6368  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6369  }
6370 
6371  } else if (sqrt_s == 0.380) {
6372 
6373  C1 = 0.0069; // Use same as 350 GeV
6374 
6375  if (Pol_em == 80. && Pol_ep == -30.){
6376  mu +=
6377  +121392. * CiHbox / LambdaNP2
6378  -68799.8 * CiHL1_11 / LambdaNP2
6379  -54383.2 * CiHe_11 / LambdaNP2
6380  -68799.8 * CiHL3_11 / LambdaNP2
6381  +57427.7 * CiHD / LambdaNP2
6382  +439155. * CiHB / LambdaNP2
6383  +76978.2 * CiHW / LambdaNP2
6384  +392293. * CiHWB / LambdaNP2
6385  -36175.9 * CiDHB / LambdaNP2
6386  -3193.74 * CiDHW / LambdaNP2
6387  -0.11 * DeltaGF()
6388  ;
6389 
6390  // Add modifications due to small variations of the SM parameters
6391  mu += cHSM * ( -2.74 * deltaMz()
6392  -1.62 * deltaMh()
6393  +2.907 * deltaaMZ()
6394  +0.079 * deltaGmu() );
6395 
6396  } else if (Pol_em == -80. && Pol_ep == 30.){
6397  mu +=
6398  +121306. * CiHbox / LambdaNP2
6399  +80159.7 * CiHL1_11 / LambdaNP2
6400  +58002.2 * CiHe_11 / LambdaNP2
6401  +80159.7 * CiHL3_11 / LambdaNP2
6402  -123524. * CiHD / LambdaNP2
6403  +151617. * CiHB / LambdaNP2
6404  +154342. * CiHW / LambdaNP2
6405  -500961. * CiHWB / LambdaNP2
6406  +20509.9 * CiDHB / LambdaNP2
6407  -35718.1 * CiDHW / LambdaNP2
6408  -6.064 * DeltaGF()
6409  ;
6410 
6411  // Add modifications due to small variations of the SM parameters
6412  mu += cHSM * ( +9.254 * deltaMz()
6413  -1.608 * deltaMh()
6414  -3.07 * deltaaMZ()
6415  +6.04 * deltaGmu() );
6416 
6417  } else if (Pol_em == 80. && Pol_ep == 0.){
6418  mu +=
6419  +121171. * CiHbox / LambdaNP2
6420  -89494.3 * CiHL1_11 / LambdaNP2
6421  +11882.3 * CiHe_11 / LambdaNP2
6422  -89494.3 * CiHL3_11 / LambdaNP2
6423  +32430.1 * CiHD / LambdaNP2
6424  +524620. * CiHB / LambdaNP2
6425  +111520. * CiHW / LambdaNP2
6426  +156122. * CiHWB / LambdaNP2
6427  -29271.1 * CiDHB / LambdaNP2
6428  -8056.8 * CiDHW / LambdaNP2
6429  -0.928 * DeltaGF()
6430  ;
6431 
6432  // Add modifications due to small variations of the SM parameters
6433  mu += cHSM * ( -1.145 * deltaMz()
6434  -1.643 * deltaMh()
6435  +2.077 * deltaaMZ()
6436  +0.898 * deltaGmu() );
6437 
6438  } else if (Pol_em == -80. && Pol_ep == 0.){
6439  mu +=
6440  +121286. * CiHbox / LambdaNP2
6441  +30046.7 * CiHL1_11 / LambdaNP2
6442  +84014. * CiHe_11 / LambdaNP2
6443  +30046.7 * CiHL3_11 / LambdaNP2
6444  -101539. * CiHD / LambdaNP2
6445  +286981. * CiHB / LambdaNP2
6446  +164662. * CiHW / LambdaNP2
6447  -480410. * CiHWB / LambdaNP2
6448  +13149.6 * CiDHB / LambdaNP2
6449  -31886.7 * CiDHW / LambdaNP2
6450  -5.346 * DeltaGF()
6451  ;
6452 
6453  // Add modifications due to small variations of the SM parameters
6454  mu += cHSM * ( +7.766 * deltaMz()
6455  -1.629 * deltaMh()
6456  -2.353 * deltaaMZ()
6457  +5.316 * deltaGmu() );
6458 
6459  } else {
6460  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6461  }
6462 
6463  } else if (sqrt_s == 0.500) {
6464 
6465  C1 = 0.0067;
6466 
6467  if (Pol_em == 80. && Pol_ep == -30.){
6468  mu +=
6469  +121372. * CiHbox / LambdaNP2
6470  -121062. * CiHL1_11 / LambdaNP2
6471  +224754. * CiHe_11 / LambdaNP2
6472  -121062. * CiHL3_11 / LambdaNP2
6473  +55161.7 * CiHD / LambdaNP2
6474  +201238. * CiHB / LambdaNP2
6475  +52456.6 * CiHW / LambdaNP2
6476  +335517. * CiHWB / LambdaNP2
6477  -63733.4 * CiDHB / LambdaNP2
6478  -2379.21 * CiDHW / LambdaNP2
6479  -0.207 * DeltaGF()
6480  ;
6481 
6482  // Add modifications due to small variations of the SM parameters
6483  mu += cHSM * ( -2.453 * deltaMz()
6484  -1.136 * deltaMh()
6485  +2.81 * deltaaMZ()
6486  +0.175 * deltaGmu() );
6487 
6488  } else if (Pol_em == -80. && Pol_ep == 30.){
6489  mu +=
6490  +121399. * CiHbox / LambdaNP2
6491  -200849. * CiHL1_11 / LambdaNP2
6492  +96427.7 * CiHe_11 / LambdaNP2
6493  -200849. * CiHL3_11 / LambdaNP2
6494  -121178. * CiHD / LambdaNP2
6495  +83220.9 * CiHB / LambdaNP2
6496  +42832.2 * CiHW / LambdaNP2
6497  -464173. * CiHWB / LambdaNP2
6498  +37654.2 * CiDHB / LambdaNP2
6499  -59029.6 * CiDHW / LambdaNP2
6500  -6.025 * DeltaGF()
6501  ;
6502 
6503  // Add modifications due to small variations of the SM parameters
6504  mu += cHSM * ( +9.205 * deltaMz()
6505  -1.133 * deltaMh()
6506  -3.019 * deltaaMZ()
6507  +5.99 * deltaGmu() );
6508 
6509  } else if (Pol_em == 80. && Pol_ep == 0.){
6510  mu +=
6511  +121435. * CiHbox / LambdaNP2
6512  -154953. * CiHL1_11 / LambdaNP2
6513  +235326. * CiHe_11 / LambdaNP2
6514  -154953. * CiHL3_11 / LambdaNP2
6515  +30472. * CiHD / LambdaNP2
6516  +298145. * CiHB / LambdaNP2
6517  +75047.6 * CiHW / LambdaNP2
6518  +137304. * CiHWB / LambdaNP2
6519  -49636.1 * CiDHB / LambdaNP2
6520  -10277.1 * CiDHW / LambdaNP2
6521  -1.027 * DeltaGF()
6522  ;
6523 
6524  // Add modifications due to small variations of the SM parameters
6525  mu += cHSM * ( -0.829 * deltaMz()
6526  -1.142 * deltaMh()
6527  +1.988 * deltaaMZ()
6528  +0.989 * deltaGmu() );
6529 
6530  } else if (Pol_em == -80. && Pol_ep == 0.){
6531  mu +=
6532  +121468. * CiHbox / LambdaNP2
6533  -208577. * CiHL1_11 / LambdaNP2
6534  +134790. * CiHe_11 / LambdaNP2
6535  -208577. * CiHL3_11 / LambdaNP2
6536  -98708.1 * CiHD / LambdaNP2
6537  +190310. * CiHB / LambdaNP2
6538  +62321.4 * CiHW / LambdaNP2
6539  -429412. * CiHWB / LambdaNP2
6540  +24628.2 * CiDHB / LambdaNP2
6541  -51722.9 * CiDHW / LambdaNP2
6542  -5.287 * DeltaGF()
6543  ;
6544 
6545  // Add modifications due to small variations of the SM parameters
6546  mu += cHSM * ( +7.714 * deltaMz()
6547  -1.14 * deltaMh()
6548  -2.279 * deltaaMZ()
6549  +5.251 * deltaGmu() );
6550 
6551  } else {
6552  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6553  }
6554 
6555  } else if (sqrt_s == 1.0) {
6556 
6557  C1 = 0.0065;
6558 
6559  if (Pol_em == 80. && Pol_ep == -30.){
6560  mu +=
6561  +121044. * CiHbox / LambdaNP2
6562  -206156. * CiHL1_11 / LambdaNP2
6563  +586357. * CiHe_11 / LambdaNP2
6564  -206156. * CiHL3_11 / LambdaNP2
6565  +54157.3 * CiHD / LambdaNP2
6566  -30839.6 * CiHB / LambdaNP2
6567  +18110.3 * CiHW / LambdaNP2
6568  +345253. * CiHWB / LambdaNP2
6569  -108488. * CiDHB / LambdaNP2
6570  -12324.2 * CiDHW / LambdaNP2
6571  -0.229 * DeltaGF()
6572  ;
6573 
6574  // Add modifications due to small variations of the SM parameters
6575  mu += cHSM * ( -2.141 * deltaMz()
6576  -0.544 * deltaMh()
6577  +2.775 * deltaaMZ()
6578  +0.211 * deltaGmu() );
6579 
6580  } else if (Pol_em == -80. && Pol_ep == 30.){
6581  mu +=
6582  +121085. * CiHbox / LambdaNP2
6583  -565700. * CiHL1_11 / LambdaNP2
6584  +157498. * CiHe_11 / LambdaNP2
6585  -565700. * CiHL3_11 / LambdaNP2
6586  -120795. * CiHD / LambdaNP2
6587  +7953.6 * CiHB / LambdaNP2
6588  -79908.9 * CiHW / LambdaNP2
6589  -402278. * CiHWB / LambdaNP2
6590  +54805.3 * CiDHB / LambdaNP2
6591  -101988. * CiDHW / LambdaNP2
6592  -6.001 * DeltaGF()
6593  ;
6594 
6595  // Add modifications due to small variations of the SM parameters
6596  mu += cHSM * ( +9.412 * deltaMz()
6597  -0.546 * deltaMh()
6598  -3.005 * deltaaMZ()
6599  +5.986 * deltaGmu() );
6600 
6601  } else if (Pol_em == 80. && Pol_ep == -20.){
6602  mu +=
6603  +121091. * CiHbox / LambdaNP2
6604  -225779. * CiHL1_11 / LambdaNP2
6605  +568149. * CiHe_11 / LambdaNP2
6606  -225779. * CiHL3_11 / LambdaNP2
6607  +45736.7 * CiHD / LambdaNP2
6608  +2164.38 * CiHB / LambdaNP2
6609  +20504.6 * CiHW / LambdaNP2
6610  +290141. * CiHWB / LambdaNP2
6611  -100416. * CiDHB / LambdaNP2
6612  -16574.6 * CiDHW / LambdaNP2
6613  -0.51 * DeltaGF()
6614  ;
6615 
6616  // Add modifications due to small variations of the SM parameters
6617  mu += cHSM * ( -1.569 * deltaMz()
6618  -0.555 * deltaMh()
6619  +2.507 * deltaaMZ()
6620  +0.493 * deltaGmu() );
6621 
6622  } else if (Pol_em == -80. && Pol_ep == 20.){
6623  mu +=
6624  +121091. * CiHbox / LambdaNP2
6625  -552286. * CiHL1_11 / LambdaNP2
6626  +177286. * CiHe_11 / LambdaNP2
6627  -552286. * CiHL3_11 / LambdaNP2
6628  -113484. * CiHD / LambdaNP2
6629  +29757.9 * CiHB / LambdaNP2
6630  -69897.4 * CiHW / LambdaNP2
6631  -385087. * CiHWB / LambdaNP2
6632  +47999.3 * CiDHB / LambdaNP2
6633  -98310.4 * CiDHW / LambdaNP2
6634  -5.76 * DeltaGF()
6635  ;
6636 
6637  // Add modifications due to small variations of the SM parameters
6638  mu += cHSM * ( +8.942 * deltaMz()
6639  -0.556 * deltaMh()
6640  -2.75 * deltaaMZ()
6641  +5.748 * deltaGmu() );
6642 
6643  } else if (Pol_em == 80. && Pol_ep == 0.){
6644  mu +=
6645  +120996. * CiHbox / LambdaNP2
6646  -263143. * CiHL1_11 / LambdaNP2
6647  +533190. * CiHe_11 / LambdaNP2
6648  -263143. * CiHL3_11 / LambdaNP2
6649  +29434.5 * CiHD / LambdaNP2
6650  +63176.5 * CiHB / LambdaNP2
6651  +26728.5 * CiHW / LambdaNP2
6652  +184228. * CiHWB / LambdaNP2
6653  -85487.1 * CiDHB / LambdaNP2
6654  -24906.1 * CiDHW / LambdaNP2
6655  -1.044 * DeltaGF()
6656  ;
6657 
6658  // Add modifications due to small variations of the SM parameters
6659  mu += cHSM * ( -0.508 * deltaMz()
6660  -0.545 * deltaMh()
6661  +1.958 * deltaaMZ()
6662  +1.027 * deltaGmu() );
6663 
6664  } else if (Pol_em == -80. && Pol_ep == 0.){
6665  mu +=
6666  +121114. * CiHbox / LambdaNP2
6667  -524119. * CiHL1_11 / LambdaNP2
6668  +218758. * CiHe_11 / LambdaNP2
6669  -524119. * CiHL3_11 / LambdaNP2
6670  -98164. * CiHD / LambdaNP2
6671  +74694.7 * CiHB / LambdaNP2
6672  -49060.4 * CiHW / LambdaNP2
6673  -348619. * CiHWB / LambdaNP2
6674  +33861.6 * CiDHB / LambdaNP2
6675  -90369.8 * CiDHW / LambdaNP2
6676  -5.256 * DeltaGF()
6677  ;
6678 
6679  // Add modifications due to small variations of the SM parameters
6680  mu += cHSM * ( +7.922 * deltaMz()
6681  -0.546 * deltaMh()
6682  -2.261 * deltaaMZ()
6683  +5.242 * deltaGmu() );
6684 
6685  } else {
6686  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6687  }
6688 
6689  } else if (sqrt_s == 1.4) {
6690 
6691  C1 = 0.0065;
6692 
6693  if (Pol_em == 80. && Pol_ep == -30.){
6694  mu +=
6695  +120762. * CiHbox / LambdaNP2
6696  -242720. * CiHL1_11 / LambdaNP2
6697  +714345. * CiHe_11 / LambdaNP2
6698  -242720. * CiHL3_11 / LambdaNP2
6699  +53823.3 * CiHD / LambdaNP2
6700  -64876.7 * CiHB / LambdaNP2
6701  +9362.37 * CiHW / LambdaNP2
6702  +355440. * CiHWB / LambdaNP2
6703  -127361. * CiDHB / LambdaNP2
6704  -18147.3 * CiDHW / LambdaNP2
6705  -0.228 * DeltaGF()
6706  ;
6707 
6708  // Add modifications due to small variations of the SM parameters
6709  mu += cHSM * ( -2.05 * deltaMz()
6710  -0.422 * deltaMh()
6711  +2.78 * deltaaMZ()
6712  +0.2 * deltaGmu() );
6713 
6714  } else if (Pol_em == -80. && Pol_ep == 30.){
6715  mu +=
6716  +120818. * CiHbox / LambdaNP2
6717  -692905. * CiHL1_11 / LambdaNP2
6718  +184416. * CiHe_11 / LambdaNP2
6719  -692905. * CiHL3_11 / LambdaNP2
6720  -121143. * CiHD / LambdaNP2
6721  -4989.81 * CiHB / LambdaNP2
6722  -93241.6 * CiHW / LambdaNP2
6723  -392394. * CiHWB / LambdaNP2
6724  +60556.9 * CiDHB / LambdaNP2
6725  -121409. * CiDHW / LambdaNP2
6726  -6.003 * DeltaGF()
6727  ;
6728 
6729  // Add modifications due to small variations of the SM parameters
6730  mu += cHSM * ( +9.501 * deltaMz()
6731  -0.422 * deltaMh()
6732  -2.999 * deltaaMZ()
6733  +5.972 * deltaGmu() );
6734 
6735  } else if (Pol_em == 80. && Pol_ep == 0.){
6736  mu +=
6737  +120773. * CiHbox / LambdaNP2
6738  -309806. * CiHL1_11 / LambdaNP2
6739  +643900. * CiHe_11 / LambdaNP2
6740  -309806. * CiHL3_11 / LambdaNP2
6741  +29091.1 * CiHD / LambdaNP2
6742  +22438.3 * CiHB / LambdaNP2
6743  +16021.7 * CiHW / LambdaNP2
6744  +202496. * CiHWB / LambdaNP2
6745  -100775. * CiDHB / LambdaNP2
6746  -32830.8 * CiDHW / LambdaNP2
6747  -1.043 * DeltaGF()
6748  ;
6749 
6750  // Add modifications due to small variations of the SM parameters
6751  mu += cHSM * ( -0.415 * deltaMz()
6752  -0.422 * deltaMh()
6753  +1.961 * deltaaMZ()
6754  +1.014 * deltaGmu() );
6755 
6756  } else if (Pol_em == -80. && Pol_ep == 0.){
6757  mu +=
6758  +120795. * CiHbox / LambdaNP2
6759  -637584. * CiHL1_11 / LambdaNP2
6760  +256188. * CiHe_11 / LambdaNP2
6761  -637584. * CiHL3_11 / LambdaNP2
6762  -98543.3 * CiHD / LambdaNP2
6763  +49040.2 * CiHB / LambdaNP2
6764  -63051.7 * CiHW / LambdaNP2
6765  -332850. * CiHWB / LambdaNP2
6766  +36510.1 * CiDHB / LambdaNP2
6767  -108018. * CiDHW / LambdaNP2
6768  -5.256 * DeltaGF()
6769  ;
6770 
6771  // Add modifications due to small variations of the SM parameters
6772  mu += cHSM * ( +8.01 * deltaMz()
6773  -0.423 * deltaMh()
6774  -2.255 * deltaaMZ()
6775  +5.227 * deltaGmu() );
6776 
6777  } else {
6778  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6779  }
6780 
6781  } else if (sqrt_s == 1.5) {
6782 
6783  C1 = 0.0065;// Use the same as 1400 GeV
6784 
6785  if (Pol_em == 80. && Pol_ep == -30.){
6786  mu +=
6787  +120570. * CiHbox / LambdaNP2
6788  -250340. * CiHL1_11 / LambdaNP2
6789  +739684. * CiHe_11 / LambdaNP2
6790  -250340. * CiHL3_11 / LambdaNP2
6791  +53685.8 * CiHD / LambdaNP2
6792  -71192.9 * CiHB / LambdaNP2
6793  +9743.41 * CiHW / LambdaNP2
6794  +357556. * CiHWB / LambdaNP2
6795  -131206. * CiDHB / LambdaNP2
6796  -19448. * CiDHW / LambdaNP2
6797  -0.224 * DeltaGF()
6798  ;
6799 
6800  // Add modifications due to small variations of the SM parameters
6801  mu += cHSM * ( -2.032 * deltaMz()
6802  -0.4 * deltaMh()
6803  +2.778 * deltaaMZ()
6804  +0.194 * deltaGmu() );
6805 
6806  } else if (Pol_em == -80. && Pol_ep == 30.){
6807  mu +=
6808  +120602. * CiHbox / LambdaNP2
6809  -718001. * CiHL1_11 / LambdaNP2
6810  +189852. * CiHe_11 / LambdaNP2
6811  -718001. * CiHL3_11 / LambdaNP2
6812  -121214. * CiHD / LambdaNP2
6813  -6057.91 * CiHB / LambdaNP2
6814  -95148.1 * CiHW / LambdaNP2
6815  -390958. * CiHWB / LambdaNP2
6816  +61690.7 * CiDHB / LambdaNP2
6817  -125382. * CiDHW / LambdaNP2
6818  -5.997 * DeltaGF()
6819  ;
6820 
6821  // Add modifications due to small variations of the SM parameters
6822  mu += cHSM * ( +9.519 * deltaMz()
6823  -0.399 * deltaMh()
6824  -3.001 * deltaaMZ()
6825  +5.965 * deltaGmu() );
6826 
6827  } else if (Pol_em == 80. && Pol_ep == 0.){
6828  mu +=
6829  +120563. * CiHbox / LambdaNP2
6830  -319378. * CiHL1_11 / LambdaNP2
6831  +665765. * CiHe_11 / LambdaNP2
6832  -319378. * CiHL3_11 / LambdaNP2
6833  +29010.7 * CiHD / LambdaNP2
6834  +14190.4 * CiHB / LambdaNP2
6835  +16080. * CiHW / LambdaNP2
6836  +205187. * CiHWB / LambdaNP2
6837  -103927. * CiDHB / LambdaNP2
6838  -34420.2 * CiDHW / LambdaNP2
6839  -1.04 * DeltaGF()
6840  ;
6841 
6842  // Add modifications due to small variations of the SM parameters
6843  mu += cHSM * ( -0.398 * deltaMz()
6844  -0.4 * deltaMh()
6845  +1.96 * deltaaMZ()
6846  +1.01 * deltaGmu() );
6847 
6848  } else if (Pol_em == -80. && Pol_ep == 0.){
6849  mu +=
6850  +120607. * CiHbox / LambdaNP2
6851  -659879. * CiHL1_11 / LambdaNP2
6852  +263841. * CiHe_11 / LambdaNP2
6853  -659879. * CiHL3_11 / LambdaNP2
6854  -98617.3 * CiHD / LambdaNP2
6855  +46418.4 * CiHB / LambdaNP2
6856  -64166.6 * CiHW / LambdaNP2
6857  -330855. * CiHWB / LambdaNP2
6858  +36774.5 * CiDHB / LambdaNP2
6859  -111573. * CiDHW / LambdaNP2
6860  -5.253 * DeltaGF()
6861  ;
6862 
6863  // Add modifications due to small variations of the SM parameters
6864  mu += cHSM * ( +8.03 * deltaMz()
6865  -0.4 * deltaMh()
6866  -2.257 * deltaaMZ()
6867  +5.221 * deltaGmu() );
6868 
6869  } else {
6870  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6871  }
6872 
6873  } else if (sqrt_s == 3.0) {
6874 
6875  C1 = 0.0063;
6876 
6877  if (Pol_em == 80. && Pol_ep == -30.){
6878  mu +=
6879  +120539. * CiHbox / LambdaNP2
6880  -327096. * CiHL1_11 / LambdaNP2
6881  +988310. * CiHe_11 / LambdaNP2
6882  -327096. * CiHL3_11 / LambdaNP2
6883  +53758.1 * CiHD / LambdaNP2
6884  -79161. * CiHB / LambdaNP2
6885  +3856.87 * CiHW / LambdaNP2
6886  +369878. * CiHWB / LambdaNP2
6887  -170059. * CiDHB / LambdaNP2
6888  -32235.8 * CiDHW / LambdaNP2
6889  -0.226 * DeltaGF()
6890  ;
6891 
6892  // Add modifications due to small variations of the SM parameters
6893  mu += cHSM * ( -1.896 * deltaMz()
6894  -0.264 * deltaMh()
6895  +2.778 * deltaaMZ()
6896  +0.174 * deltaGmu() );
6897 
6898  } else if (Pol_em == -80. && Pol_ep == 30.){
6899  mu +=
6900  +120565. * CiHbox / LambdaNP2
6901  -961658. * CiHL1_11 / LambdaNP2
6902  +247947. * CiHe_11 / LambdaNP2
6903  -961658. * CiHL3_11 / LambdaNP2
6904  -121230. * CiHD / LambdaNP2
6905  -10752.9 * CiHB / LambdaNP2
6906  -92123.7 * CiHW / LambdaNP2
6907  -391807. * CiHWB / LambdaNP2
6908  +73242.2 * CiDHB / LambdaNP2
6909  -165690. * CiDHW / LambdaNP2
6910  -6.002 * DeltaGF()
6911  ;
6912 
6913  // Add modifications due to small variations of the SM parameters
6914  mu += cHSM * ( +9.659 * deltaMz()
6915  -0.264 * deltaMh()
6916  -3.003 * deltaaMZ()
6917  +5.943 * deltaGmu() );
6918 
6919  } else if (Pol_em == 80. && Pol_ep == 0.){
6920  mu +=
6921  +120534. * CiHbox / LambdaNP2
6922  -417962. * CiHL1_11 / LambdaNP2
6923  +884851. * CiHe_11 / LambdaNP2
6924  -417962. * CiHL3_11 / LambdaNP2
6925  +29065.5 * CiHD / LambdaNP2
6926  -10885.4 * CiHB / LambdaNP2
6927  +8249.25 * CiHW / LambdaNP2
6928  +228820. * CiHWB / LambdaNP2
6929  -135851. * CiDHB / LambdaNP2
6930  -51177.2 * CiDHW / LambdaNP2
6931  -1.04 * DeltaGF()
6932  ;
6933 
6934  // Add modifications due to small variations of the SM parameters
6935  mu += cHSM * ( -0.262 * deltaMz()
6936  -0.264 * deltaMh()
6937  +1.959 * deltaaMZ()
6938  +0.987 * deltaGmu() );
6939 
6940  } else if (Pol_em == -80. && Pol_ep == 0.){
6941  mu +=
6942  +120480. * CiHbox / LambdaNP2
6943  -880604. * CiHL1_11 / LambdaNP2
6944  +344657. * CiHe_11 / LambdaNP2
6945  -880604. * CiHL3_11 / LambdaNP2
6946  -98656.8 * CiHD / LambdaNP2
6947  +28681.4 * CiHB / LambdaNP2
6948  -66216.6 * CiHW / LambdaNP2
6949  -320715. * CiHWB / LambdaNP2
6950  +41721.6 * CiDHB / LambdaNP2
6951  -148698. * CiDHW / LambdaNP2
6952  -5.256 * DeltaGF()
6953  ;
6954 
6955  // Add modifications due to small variations of the SM parameters
6956  mu += cHSM * ( +8.169 * deltaMz()
6957  -0.264 * deltaMh()
6958  -2.259 * deltaaMZ()
6959  +5.202 * deltaGmu() );
6960 
6961  } else {
6962  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6963  }
6964 
6965  } else
6966  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZBFPol()");
6967 
6968  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
6969  //(Assume similar to WBF.)
6970  mu += eeeWBFint + eeeWBFpar;
6971 
6972 // Linear contribution from Higgs self-coupling
6973  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
6974 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
6976 
6977  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
6978 
6979  return mu;
6980 }

◆ mueeZH()

double NPSMEFTd6::mueeZH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH}\)

Reimplemented from NPbase.

Definition at line 7553 of file NPSMEFTd6.cpp.

7554 {
7555  double mu = 1.0;
7556 
7557  double C1 = 0.0;
7558 
7559  if (sqrt_s == 0.240) {
7560 
7561  C1 = 0.017;
7562 
7563  mu +=
7564  +121263. * CiHbox / LambdaNP2
7565  +898682. * CiHL1_11 / LambdaNP2
7566  -767820. * CiHe_11 / LambdaNP2
7567  +898682. * CiHL3_11 / LambdaNP2
7568  -6046.36 * CiHD / LambdaNP2
7569  +122439. * CiHB / LambdaNP2
7570  +540057. * CiHW / LambdaNP2
7571  +231063. * CiHWB / LambdaNP2
7572  +17593.2 * CiDHB / LambdaNP2
7573  +53409.5 * CiDHW / LambdaNP2
7574  -2.2 * DeltaGF()
7575  ;
7576 
7577  // Add modifications due to small variations of the SM parameters
7578  mu += cHSM * ( -0.2 * deltaaMZ()
7579  +2.2 * deltaGmu()
7580  +4.775 * deltaMz()
7581  -3.071 * deltaMh() );
7582 
7583  if (FlagQuadraticTerms) {
7584  //Add contributions that are quadratic in the effective coefficients
7585  mu += 0.0;
7586  }
7587 
7588  } else if (sqrt_s == 0.250) {
7589 
7590  C1 = 0.015;
7591 
7592  mu +=
7593  +121263. * CiHbox / LambdaNP2
7594  +975101. * CiHL1_11 / LambdaNP2
7595  -833750. * CiHe_11 / LambdaNP2
7596  +975101. * CiHL3_11 / LambdaNP2
7597  -6046.36 * CiHD / LambdaNP2
7598  +128443. * CiHB / LambdaNP2
7599  +568273. * CiHW / LambdaNP2
7600  +244206. * CiHWB / LambdaNP2
7601  +19818.6 * CiDHB / LambdaNP2
7602  +60127.6 * CiDHW / LambdaNP2
7603  -2.2 * DeltaGF()
7604  ;
7605 
7606  // Add modifications due to small variations of the SM parameters
7607  mu += cHSM * ( -0.2 * deltaaMZ()
7608  +2.2 * deltaGmu()
7609  +5.219 * deltaMz()
7610  -2.27 * deltaMh() );
7611 
7612  if (FlagQuadraticTerms) {
7613  //Add contributions that are quadratic in the effective coefficients
7614  mu += 0.0;
7615  }
7616 
7617  } else if (sqrt_s == 0.350) {
7618 
7619  C1 = 0.0057;
7620 
7621  mu +=
7622  +121283. * CiHbox / LambdaNP2
7623  +1911340. * CiHL1_11 / LambdaNP2
7624  -1640958. * CiHe_11 / LambdaNP2
7625  +1911340. * CiHL3_11 / LambdaNP2
7626  -6009.52 * CiHD / LambdaNP2
7627  +173183. * CiHB / LambdaNP2
7628  +785843. * CiHW / LambdaNP2
7629  +344494. * CiHWB / LambdaNP2
7630  +59158.7 * CiDHB / LambdaNP2
7631  +167954. * CiDHW / LambdaNP2
7632  -2.201 * DeltaGF()
7633  ;
7634 
7635  // Add modifications due to small variations of the SM parameters
7636  mu += cHSM * ( -0.2 * deltaaMZ()
7637  +2.2 * deltaGmu()
7638  +5.396 * deltaMz()
7639  -0.729 * deltaMh() );
7640 
7641  if (FlagQuadraticTerms) {
7642  //Add contributions that are quadratic in the effective coefficients
7643  mu += 0.0;
7644  }
7645 
7646  } else if (sqrt_s == 0.365) {
7647 
7648  C1 = 0.0057; // Use same as 350 GeV
7649 
7650  mu +=
7651  +121243. * CiHbox / LambdaNP2
7652  +2078482. * CiHL1_11 / LambdaNP2
7653  -1785085. * CiHe_11 / LambdaNP2
7654  +2078482. * CiHL3_11 / LambdaNP2
7655  -6010.65 * CiHD / LambdaNP2
7656  +178173. * CiHB / LambdaNP2
7657  +809806. * CiHW / LambdaNP2
7658  +355487. * CiHWB / LambdaNP2
7659  +67662.7 * CiDHB / LambdaNP2
7660  +190194. * CiDHW / LambdaNP2
7661  -2.201 * DeltaGF()
7662  ;
7663 
7664  // Add modifications due to small variations of the SM parameters
7665  mu += cHSM * ( -0.2 * deltaaMZ()
7666  +2.2 * deltaGmu()
7667  +5.348 * deltaMz()
7668  -0.664 * deltaMh() );
7669 
7670  if (FlagQuadraticTerms) {
7671  //Add contributions that are quadratic in the effective coefficients
7672  mu += 0.0;
7673  }
7674 
7675  } else if (sqrt_s == 0.380) {
7676 
7677  C1 = 0.0057; // Use same as 350 GeV
7678 
7679  mu +=
7680  +121281. * CiHbox / LambdaNP2
7681  +2253013. * CiHL1_11 / LambdaNP2
7682  -1934557. * CiHe_11 / LambdaNP2
7683  +2253013. * CiHL3_11 / LambdaNP2
7684  -6026.37 * CiHD / LambdaNP2
7685  +182674. * CiHB / LambdaNP2
7686  +832109. * CiHW / LambdaNP2
7687  +365819. * CiHWB / LambdaNP2
7688  +76742. * CiDHB / LambdaNP2
7689  +214030. * CiDHW / LambdaNP2
7690  -2.202 * DeltaGF()
7691  ;
7692 
7693  // Add modifications due to small variations of the SM parameters
7694  mu += cHSM * ( -0.2 * deltaaMZ()
7695  +2.2 * deltaGmu()
7696  +5.301 * deltaMz()
7697  -0.609 * deltaMh() );
7698 
7699  if (FlagQuadraticTerms) {
7700  //Add contributions that are quadratic in the effective coefficients
7701  mu += 0.0;
7702  }
7703 
7704  } else if (sqrt_s == 0.500) {
7705 
7706  C1 = 0.00099;
7707 
7708  mu +=
7709  +121264. * CiHbox / LambdaNP2
7710  +3900384. * CiHL1_11 / LambdaNP2
7711  -3350136. * CiHe_11 / LambdaNP2
7712  +3900384. * CiHL3_11 / LambdaNP2
7713  -6019.22 * CiHD / LambdaNP2
7714  +209229. * CiHB / LambdaNP2
7715  +959942. * CiHW / LambdaNP2
7716  +425112. * CiHWB / LambdaNP2
7717  +169841. * CiDHB / LambdaNP2
7718  +455437. * CiDHW / LambdaNP2
7719  -2.202 * DeltaGF()
7720  ;
7721 
7722  // Add modifications due to small variations of the SM parameters
7723  mu += cHSM * ( -0.2 * deltaaMZ()
7724  +2.2 * deltaGmu()
7725  +5. * deltaMz()
7726  -0.351 * deltaMh() );
7727 
7728  if (FlagQuadraticTerms) {
7729  //Add contributions that are quadratic in the effective coefficients
7730  mu += 0.0;
7731  }
7732 
7733  } else if (sqrt_s == 1.0) {
7734 
7735  C1 = -0.0012;
7736 
7737  mu +=
7738  +121274. * CiHbox / LambdaNP2
7739  +15601820. * CiHL1_11 / LambdaNP2
7740  -13395670. * CiHe_11 / LambdaNP2
7741  +15601820. * CiHL3_11 / LambdaNP2
7742  -6040.16 * CiHD / LambdaNP2
7743  +243960. * CiHB / LambdaNP2
7744  +1128805. * CiHW / LambdaNP2
7745  +503138. * CiHWB / LambdaNP2
7746  +899357. * CiDHB / LambdaNP2
7747  +2321619. * CiDHW / LambdaNP2
7748  -2.202 * DeltaGF()
7749  ;
7750 
7751  // Add modifications due to small variations of the SM parameters
7752  mu += cHSM * ( -0.2 * deltaaMZ()
7753  +2.2 * deltaGmu()
7754  +4.574 * deltaMz()
7755  -0.092 * deltaMh() );
7756 
7757  if (FlagQuadraticTerms) {
7758  //Add contributions that are quadratic in the effective coefficients
7759  mu += 0.0;
7760  }
7761 
7762  } else if (sqrt_s == 1.4) {
7763 
7764  C1 = -0.0011;
7765 
7766  mu +=
7767  +121283. * CiHbox / LambdaNP2
7768  +30579278. * CiHL1_11 / LambdaNP2
7769  -26253064. * CiHe_11 / LambdaNP2
7770  +30579278. * CiHL3_11 / LambdaNP2
7771  -6010.77 * CiHD / LambdaNP2
7772  +250804. * CiHB / LambdaNP2
7773  +1161208. * CiHW / LambdaNP2
7774  +518040. * CiHWB / LambdaNP2
7775  +1848758. * CiDHB / LambdaNP2
7776  +4747422. * CiDHW / LambdaNP2
7777  -2.203 * DeltaGF()
7778  ;
7779 
7780  // Add modifications due to small variations of the SM parameters
7781  mu += cHSM * ( -0.2 * deltaaMZ()
7782  +2.2 * deltaGmu()
7783  +4.491 * deltaMz()
7784  -0.047 * deltaMh() );
7785 
7786  if (FlagQuadraticTerms) {
7787  //Add contributions that are quadratic in the effective coefficients
7788  mu += 0.0;
7789  }
7790 
7791  } else if (sqrt_s == 1.5) {
7792 
7793  C1 = -0.0011;// Use the same as 1400 GeV
7794 
7795  mu +=
7796  +121262. * CiHbox / LambdaNP2
7797  +35102329. * CiHL1_11 / LambdaNP2
7798  -30135878. * CiHe_11 / LambdaNP2
7799  +35102329. * CiHL3_11 / LambdaNP2
7800  -6034.22 * CiHD / LambdaNP2
7801  +251576. * CiHB / LambdaNP2
7802  +1165634. * CiHW / LambdaNP2
7803  +519954. * CiHWB / LambdaNP2
7804  +2132554. * CiDHB / LambdaNP2
7805  +5481906. * CiDHW / LambdaNP2
7806  -2.203 * DeltaGF()
7807  ;
7808 
7809  // Add modifications due to small variations of the SM parameters
7810  mu += cHSM * ( -0.2 * deltaaMZ()
7811  +2.2 * deltaGmu()
7812  +4.479 * deltaMz()
7813  -0.041 * deltaMh() );
7814 
7815  if (FlagQuadraticTerms) {
7816  //Add contributions that are quadratic in the effective coefficients
7817  mu += 0.0;
7818  }
7819 
7820  } else if (sqrt_s == 3.0) {
7821 
7822  C1 = -0.00054;
7823 
7824  mu +=
7825  +121279. * CiHbox / LambdaNP2
7826  +140413697. * CiHL1_11 / LambdaNP2
7827  -120540988. * CiHe_11 / LambdaNP2
7828  +140413697. * CiHL3_11 / LambdaNP2
7829  -6012.61 * CiHD / LambdaNP2
7830  +257222. * CiHB / LambdaNP2
7831  +1188444. * CiHW / LambdaNP2
7832  +530503. * CiHWB / LambdaNP2
7833  +8839419. * CiDHB / LambdaNP2
7834  +22583370. * CiDHW / LambdaNP2
7835  -2.202 * DeltaGF()
7836  ;
7837 
7838  // Add modifications due to small variations of the SM parameters
7839  mu += cHSM * ( -0.2 * deltaaMZ()
7840  +2.2 * deltaGmu()
7841  +4.42 * deltaMz()
7842  -0.01 * deltaMh() );
7843 
7844  if (FlagQuadraticTerms) {
7845  //Add contributions that are quadratic in the effective coefficients
7846  mu += 0.0;
7847  }
7848 
7849  } else
7850  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZH()");
7851 
7852  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7853  mu += eeeZHint + eeeZHpar;
7854 
7855 // Linear contribution from Higgs self-coupling
7856  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
7857 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
7859 
7860  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7861 
7862  return mu;
7863 }

◆ mueeZHPol()

double NPSMEFTd6::mueeZHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH}\)

Reimplemented from NPbase.

Definition at line 7910 of file NPSMEFTd6.cpp.

7911 {
7912  double mu = 1.0;
7913 
7914  double C1 = 0.0;
7915 
7916  if (sqrt_s == 0.240) {
7917 
7918  C1 = 0.017;
7919 
7920  if (Pol_em == 80. && Pol_ep == -30.){
7921  mu +=
7922  +121260. * CiHbox / LambdaNP2
7923  +117191. * CiHL1_11 / LambdaNP2
7924  -1681596. * CiHe_11 / LambdaNP2
7925  +117191. * CiHL3_11 / LambdaNP2
7926  +74555.1 * CiHD / LambdaNP2
7927  +528105. * CiHB / LambdaNP2
7928  +134403. * CiHW / LambdaNP2
7929  +872560. * CiHWB / LambdaNP2
7930  +137571. * CiDHB / LambdaNP2
7931  -12321.5 * CiDHW / LambdaNP2
7932  +0.459 * DeltaGF()
7933  ;
7934 
7935  // Add modifications due to small variations of the SM parameters
7936  mu += cHSM * ( +2.46 * deltaaMZ()
7937  -0.46 * deltaGmu()
7938  -0.544 * deltaMz()
7939  -3.071 * deltaMh() );
7940 
7941  } else if (Pol_em == -80. && Pol_ep == 30.){
7942  mu +=
7943  +121254. * CiHbox / LambdaNP2
7944  +1495015. * CiHL1_11 / LambdaNP2
7945  -76567.2 * CiHe_11 / LambdaNP2
7946  +1495015. * CiHL3_11 / LambdaNP2
7947  -67582.1 * CiHD / LambdaNP2
7948  -187104. * CiHB / LambdaNP2
7949  +849552. * CiHW / LambdaNP2
7950  -258537. * CiHWB / LambdaNP2
7951  -73970.1 * CiDHB / LambdaNP2
7952  +103582. * CiDHW / LambdaNP2
7953  -4.23 * DeltaGF()
7954  ;
7955 
7956  // Add modifications due to small variations of the SM parameters
7957  mu += cHSM * ( -2.23 * deltaaMZ()
7958  +4.23 * deltaGmu()
7959  +8.834 * deltaMz()
7960  -3.071 * deltaMh() );
7961 
7962  } else if (Pol_em == 80. && Pol_ep == 0.){
7963  mu +=
7964  +121256. * CiHbox / LambdaNP2
7965  +204529. * CiHL1_11 / LambdaNP2
7966  -1578998. * CiHe_11 / LambdaNP2
7967  +204529. * CiHL3_11 / LambdaNP2
7968  +65548.7 * CiHD / LambdaNP2
7969  +482729. * CiHB / LambdaNP2
7970  +179733. * CiHW / LambdaNP2
7971  +800870. * CiHWB / LambdaNP2
7972  +124170. * CiDHB / LambdaNP2
7973  -5016.48 * CiDHW / LambdaNP2
7974  +0.162 * DeltaGF()
7975  ;
7976 
7977  // Add modifications due to small variations of the SM parameters
7978  mu += cHSM * ( +2.163 * deltaaMZ()
7979  -0.163 * deltaGmu()
7980  +0.05 * deltaMz()
7981  -3.071 * deltaMh() );
7982 
7983  } else if (Pol_em == -80. && Pol_ep == 0.){
7984  mu +=
7985  +121264. * CiHbox / LambdaNP2
7986  +1442776. * CiHL1_11 / LambdaNP2
7987  -137405. * CiHe_11 / LambdaNP2
7988  +1442776. * CiHL3_11 / LambdaNP2
7989  -62167.6 * CiHD / LambdaNP2
7990  -159988. * CiHB / LambdaNP2
7991  +822448. * CiHW / LambdaNP2
7992  -215639. * CiHWB / LambdaNP2
7993  -65950.1 * CiDHB / LambdaNP2
7994  +99206.1 * CiDHW / LambdaNP2
7995  -4.052 * DeltaGF()
7996  ;
7997 
7998  // Add modifications due to small variations of the SM parameters
7999  mu += cHSM * ( -2.052 * deltaaMZ()
8000  +4.052 * deltaGmu()
8001  +8.479 * deltaMz()
8002  -3.071 * deltaMh() );
8003 
8004  } else {
8005  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8006  }
8007 
8008  } else if (sqrt_s == 0.250) {
8009 
8010  C1 = 0.015;
8011 
8012  if (Pol_em == 80. && Pol_ep == -30.){
8013  mu +=
8014  +121264. * CiHbox / LambdaNP2
8015  +127210. * CiHL1_11 / LambdaNP2
8016  -1824910. * CiHe_11 / LambdaNP2
8017  +127210. * CiHL3_11 / LambdaNP2
8018  +74597.1 * CiHD / LambdaNP2
8019  +560319. * CiHB / LambdaNP2
8020  +136129. * CiHW / LambdaNP2
8021  +902676. * CiHWB / LambdaNP2
8022  +154358. * CiDHB / LambdaNP2
8023  -13612.9 * CiDHW / LambdaNP2
8024  +0.459 * DeltaGF()
8025  ;
8026 
8027  // Add modifications due to small variations of the SM parameters
8028  mu += cHSM * ( +2.46 * deltaaMZ()
8029  -0.46 * deltaGmu()
8030  -0.1 * deltaMz()
8031  -2.27 * deltaMh() );
8032 
8033  } else if (Pol_em == -80. && Pol_ep == 30.){
8034  mu +=
8035  +121257. * CiHbox / LambdaNP2
8036  +1622228. * CiHL1_11 / LambdaNP2
8037  -83107. * CiHe_11 / LambdaNP2
8038  +1622228. * CiHL3_11 / LambdaNP2
8039  -67554.3 * CiHD / LambdaNP2
8040  -201409. * CiHB / LambdaNP2
8041  +898116. * CiHW / LambdaNP2
8042  -258306. * CiHWB / LambdaNP2
8043  -82898. * CiDHB / LambdaNP2
8044  +116421. * CiDHW / LambdaNP2
8045  -4.23 * DeltaGF()
8046  ;
8047 
8048  // Add modifications due to small variations of the SM parameters
8049  mu += cHSM * ( -2.23 * deltaaMZ()
8050  +4.23 * deltaGmu()
8051  +9.279 * deltaMz()
8052  -2.27 * deltaMh() );
8053 
8054  } else if (Pol_em == 80. && Pol_ep == 0.){
8055  mu +=
8056  +121309. * CiHbox / LambdaNP2
8057  +221930. * CiHL1_11 / LambdaNP2
8058  -1714047. * CiHe_11 / LambdaNP2
8059  +221930. * CiHL3_11 / LambdaNP2
8060  +65599.6 * CiHD / LambdaNP2
8061  +512136. * CiHB / LambdaNP2
8062  +184424. * CiHW / LambdaNP2
8063  +829145. * CiHWB / LambdaNP2
8064  +139369. * CiDHB / LambdaNP2
8065  -5351.17 * CiDHW / LambdaNP2
8066  +0.162 * DeltaGF()
8067  ;
8068 
8069  // Add modifications due to small variations of the SM parameters
8070  mu += cHSM * ( +2.163 * deltaaMZ()
8071  -0.163 * deltaGmu()
8072  +0.494 * deltaMz()
8073  -2.27 * deltaMh() );
8074 
8075  } else if (Pol_em == -80. && Pol_ep == 0.){
8076  mu +=
8077  +121269. * CiHbox / LambdaNP2
8078  +1565559. * CiHL1_11 / LambdaNP2
8079  -148908. * CiHe_11 / LambdaNP2
8080  +1565559. * CiHL3_11 / LambdaNP2
8081  -62170. * CiHD / LambdaNP2
8082  -172540. * CiHB / LambdaNP2
8083  +869218. * CiHW / LambdaNP2
8084  -214299. * CiHWB / LambdaNP2
8085  -73929.8 * CiDHB / LambdaNP2
8086  +111494. * CiDHW / LambdaNP2
8087  -4.053 * DeltaGF()
8088  ;
8089 
8090  // Add modifications due to small variations of the SM parameters
8091  mu += cHSM * ( -2.052 * deltaaMZ()
8092  +4.052 * deltaGmu()
8093  +8.923 * deltaMz()
8094  -2.27 * deltaMh() );
8095 
8096  } else {
8097  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8098  }
8099 
8100  } else if (sqrt_s == 0.350) {
8101 
8102  C1 = 0.0057;
8103 
8104  if (Pol_em == 80. && Pol_ep == -30.){
8105  mu +=
8106  +121274. * CiHbox / LambdaNP2
8107  +249309. * CiHL1_11 / LambdaNP2
8108  -3576996. * CiHe_11 / LambdaNP2
8109  +249309. * CiHL3_11 / LambdaNP2
8110  +74596.5 * CiHD / LambdaNP2
8111  +812491. * CiHB / LambdaNP2
8112  +146212. * CiHW / LambdaNP2
8113  +1135161. * CiHWB / LambdaNP2
8114  +395085. * CiDHB / LambdaNP2
8115  -16140.8 * CiDHW / LambdaNP2
8116  +0.458 * DeltaGF()
8117  ;
8118 
8119  // Add modifications due to small variations of the SM parameters
8120  mu += cHSM * ( +2.46 * deltaaMZ()
8121  -0.46 * deltaGmu()
8122  +0.077 * deltaMz()
8123  -0.729 * deltaMh() );
8124 
8125  } else if (Pol_em == -80. && Pol_ep == 30.){
8126  mu +=
8127  +121289. * CiHbox / LambdaNP2
8128  +3179548. * CiHL1_11 / LambdaNP2
8129  -163347. * CiHe_11 / LambdaNP2
8130  +3179548. * CiHL3_11 / LambdaNP2
8131  -67524.8 * CiHD / LambdaNP2
8132  -314653. * CiHB / LambdaNP2
8133  +1273817. * CiHW / LambdaNP2
8134  -258947. * CiHWB / LambdaNP2
8135  -197137. * CiDHB / LambdaNP2
8136  +308384. * CiDHW / LambdaNP2
8137  -4.231 * DeltaGF()
8138  ;
8139 
8140  // Add modifications due to small variations of the SM parameters
8141  mu += cHSM * ( -2.23 * deltaaMZ()
8142  +4.23 * deltaGmu()
8143  +9.456 * deltaMz()
8144  -0.729 * deltaMh() );
8145 
8146  } else if (Pol_em == 80. && Pol_ep == 0.){
8147  mu +=
8148  +121304. * CiHbox / LambdaNP2
8149  +434952. * CiHL1_11 / LambdaNP2
8150  -3360980. * CiHe_11 / LambdaNP2
8151  +434952. * CiHL3_11 / LambdaNP2
8152  +65624.7 * CiHD / LambdaNP2
8153  +741142. * CiHB / LambdaNP2
8154  +217654. * CiHW / LambdaNP2
8155  +1046799. * CiHWB / LambdaNP2
8156  +357606. * CiDHB / LambdaNP2
8157  +4440.1 * CiDHW / LambdaNP2
8158  +0.161 * DeltaGF()
8159  ;
8160 
8161  // Add modifications due to small variations of the SM parameters
8162  mu += cHSM * ( +2.163 * deltaaMZ()
8163  -0.163 * deltaGmu()
8164  +0.671 * deltaMz()
8165  -0.729 * deltaMh() );
8166 
8167  } else if (Pol_em == -80. && Pol_ep == 0.){
8168  mu +=
8169  +121259. * CiHbox / LambdaNP2
8170  +3068356. * CiHL1_11 / LambdaNP2
8171  -292427. * CiHe_11 / LambdaNP2
8172  +3068356. * CiHL3_11 / LambdaNP2
8173  -62160.7 * CiHD / LambdaNP2
8174  -271962. * CiHB / LambdaNP2
8175  +1231171. * CiHW / LambdaNP2
8176  -206112. * CiHWB / LambdaNP2
8177  -174718. * CiDHB / LambdaNP2
8178  +296046. * CiDHW / LambdaNP2
8179  -4.053 * DeltaGF()
8180  ;
8181 
8182  // Add modifications due to small variations of the SM parameters
8183  mu += cHSM * ( -2.052 * deltaaMZ()
8184  +4.052 * deltaGmu()
8185  +9.1 * deltaMz()
8186  -0.729 * deltaMh() );
8187 
8188  } else {
8189  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8190  }
8191 
8192  } else if (sqrt_s == 0.365) {
8193 
8194  C1 = 0.0057; // Use same as 350 GeV
8195 
8196  if (Pol_em == 80. && Pol_ep == -30.){
8197  mu +=
8198  +121270. * CiHbox / LambdaNP2
8199  +271098. * CiHL1_11 / LambdaNP2
8200  -3890169. * CiHe_11 / LambdaNP2
8201  +271098. * CiHL3_11 / LambdaNP2
8202  +74554. * CiHD / LambdaNP2
8203  +840573. * CiHB / LambdaNP2
8204  +147108. * CiHW / LambdaNP2
8205  +1160947. * CiHWB / LambdaNP2
8206  +442125. * CiDHB / LambdaNP2
8207  -15038.8 * CiDHW / LambdaNP2
8208  +0.459 * DeltaGF()
8209  ;
8210 
8211  // Add modifications due to small variations of the SM parameters
8212  mu += cHSM * ( +2.46 * deltaaMZ()
8213  -0.46 * deltaGmu()
8214  +0.029 * deltaMz()
8215  -0.664 * deltaMh() );
8216 
8217  } else if (Pol_em == -80. && Pol_ep == 30.){
8218  mu +=
8219  +121238. * CiHbox / LambdaNP2
8220  +3457848. * CiHL1_11 / LambdaNP2
8221  -177584. * CiHe_11 / LambdaNP2
8222  +3457848. * CiHL3_11 / LambdaNP2
8223  -67578.3 * CiHD / LambdaNP2
8224  -327391. * CiHB / LambdaNP2
8225  +1315671. * CiHW / LambdaNP2
8226  -259142. * CiHWB / LambdaNP2
8227  -218241. * CiDHB / LambdaNP2
8228  +346804. * CiDHW / LambdaNP2
8229  -4.231 * DeltaGF()
8230  ;
8231 
8232  // Add modifications due to small variations of the SM parameters
8233  mu += cHSM * ( -2.23 * deltaaMZ()
8234  +4.23 * deltaGmu()
8235  +9.408 * deltaMz()
8236  -0.664 * deltaMh() );
8237 
8238  } else if (Pol_em == 80. && Pol_ep == 0.){
8239  mu +=
8240  +121251. * CiHbox / LambdaNP2
8241  +472985. * CiHL1_11 / LambdaNP2
8242  -3655203. * CiHe_11 / LambdaNP2
8243  +472985. * CiHL3_11 / LambdaNP2
8244  +65559.4 * CiHD / LambdaNP2
8245  +766585. * CiHB / LambdaNP2
8246  +221202. * CiHW / LambdaNP2
8247  +1070933. * CiHWB / LambdaNP2
8248  +400293. * CiDHB / LambdaNP2
8249  +7914.02 * CiDHW / LambdaNP2
8250  +0.161 * DeltaGF()
8251  ;
8252 
8253  // Add modifications due to small variations of the SM parameters
8254  mu += cHSM * ( +2.163 * deltaaMZ()
8255  -0.163 * deltaGmu()
8256  +0.623 * deltaMz()
8257  -0.664 * deltaMh() );
8258 
8259  } else if (Pol_em == -80. && Pol_ep == 0.){
8260  mu +=
8261  +121238. * CiHbox / LambdaNP2
8262  +3336984. * CiHL1_11 / LambdaNP2
8263  -317944. * CiHe_11 / LambdaNP2
8264  +3336984. * CiHL3_11 / LambdaNP2
8265  -62188.9 * CiHD / LambdaNP2
8266  -283174. * CiHB / LambdaNP2
8267  +1271272. * CiHW / LambdaNP2
8268  -205330. * CiHWB / LambdaNP2
8269  -193153. * CiDHB / LambdaNP2
8270  +333078. * CiDHW / LambdaNP2
8271  -4.053 * DeltaGF()
8272  ;
8273 
8274  // Add modifications due to small variations of the SM parameters
8275  mu += cHSM * ( -2.052 * deltaaMZ()
8276  +4.052 * deltaGmu()
8277  +9.052 * deltaMz()
8278  -0.664 * deltaMh() );
8279 
8280  } else {
8281  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8282  }
8283 
8284  } else if (sqrt_s == 0.380) {
8285 
8286  C1 = 0.0057; // Use same as 350 GeV
8287 
8288  if (Pol_em == 80. && Pol_ep == -30.){
8289  mu +=
8290  +121228. * CiHbox / LambdaNP2
8291  +293860. * CiHL1_11 / LambdaNP2
8292  -4216491. * CiHe_11 / LambdaNP2
8293  +293860. * CiHL3_11 / LambdaNP2
8294  +74561.4 * CiHD / LambdaNP2
8295  +866754. * CiHB / LambdaNP2
8296  +147982. * CiHW / LambdaNP2
8297  +1184912. * CiHWB / LambdaNP2
8298  +492018. * CiDHB / LambdaNP2
8299  -13596.5 * CiDHW / LambdaNP2
8300  +0.459 * DeltaGF()
8301  ;
8302 
8303  // Add modifications due to small variations of the SM parameters
8304  mu += cHSM * ( +2.46 * deltaaMZ()
8305  -0.46 * deltaGmu()
8306  -0.018 * deltaMz()
8307  -0.609 * deltaMh() );
8308 
8309  } else if (Pol_em == -80. && Pol_ep == 30.){
8310  mu +=
8311  +121226. * CiHbox / LambdaNP2
8312  +3747707. * CiHL1_11 / LambdaNP2
8313  -192650. * CiHe_11 / LambdaNP2
8314  +3747707. * CiHL3_11 / LambdaNP2
8315  -67608.3 * CiHD / LambdaNP2
8316  -339193. * CiHB / LambdaNP2
8317  +1354040. * CiHW / LambdaNP2
8318  -259321. * CiHWB / LambdaNP2
8319  -240311. * CiDHB / LambdaNP2
8320  +387710. * CiDHW / LambdaNP2
8321  -4.23 * DeltaGF()
8322  ;
8323 
8324  // Add modifications due to small variations of the SM parameters
8325  mu += cHSM * ( -2.23 * deltaaMZ()
8326  +4.23 * deltaGmu()
8327  +9.361 * deltaMz()
8328  -0.609 * deltaMh() );
8329 
8330  } else if (Pol_em == 80. && Pol_ep == 0.){
8331  mu +=
8332  +121325. * CiHbox / LambdaNP2
8333  +512707. * CiHL1_11 / LambdaNP2
8334  -3961665. * CiHe_11 / LambdaNP2
8335  +512707. * CiHL3_11 / LambdaNP2
8336  +65601.7 * CiHD / LambdaNP2
8337  +790306. * CiHB / LambdaNP2
8338  +224394. * CiHW / LambdaNP2
8339  +1093297. * CiHWB / LambdaNP2
8340  +445530. * CiDHB / LambdaNP2
8341  +11860.4 * CiDHW / LambdaNP2
8342  +0.161 * DeltaGF()
8343  ;
8344 
8345  // Add modifications due to small variations of the SM parameters
8346  mu += cHSM * ( +2.163 * deltaaMZ()
8347  -0.163 * deltaGmu()
8348  +0.576 * deltaMz()
8349  -0.609 * deltaMh() );
8350 
8351  } else if (Pol_em == -80. && Pol_ep == 0.){
8352  mu +=
8353  +121273. * CiHbox / LambdaNP2
8354  +3617032. * CiHL1_11 / LambdaNP2
8355  -344629. * CiHe_11 / LambdaNP2
8356  +3617032. * CiHL3_11 / LambdaNP2
8357  -62148.3 * CiHD / LambdaNP2
8358  -293491. * CiHB / LambdaNP2
8359  +1308558. * CiHW / LambdaNP2
8360  -204594. * CiHWB / LambdaNP2
8361  -212514. * CiDHB / LambdaNP2
8362  +372554. * CiDHW / LambdaNP2
8363  -4.053 * DeltaGF()
8364  ;
8365 
8366  // Add modifications due to small variations of the SM parameters
8367  mu += cHSM * ( -2.052 * deltaaMZ()
8368  +4.052 * deltaGmu()
8369  +9.005 * deltaMz()
8370  -0.609 * deltaMh() );
8371 
8372  } else {
8373  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8374  }
8375 
8376  } else if (sqrt_s == 0.500) {
8377 
8378  C1 = 0.00099;
8379 
8380  if (Pol_em == 80. && Pol_ep == -30.){
8381  mu +=
8382  +121268. * CiHbox / LambdaNP2
8383  +508715. * CiHL1_11 / LambdaNP2
8384  -7299333. * CiHe_11 / LambdaNP2
8385  +508715. * CiHL3_11 / LambdaNP2
8386  +74603.6 * CiHD / LambdaNP2
8387  +1018069. * CiHB / LambdaNP2
8388  +151257. * CiHW / LambdaNP2
8389  +1323862. * CiHWB / LambdaNP2
8390  +985604. * CiDHB / LambdaNP2
8391  +8362.16 * CiDHW / LambdaNP2
8392  +0.458 * DeltaGF()
8393  ;
8394 
8395  // Add modifications due to small variations of the SM parameters
8396  mu += cHSM * ( +2.46 * deltaaMZ()
8397  -0.46 * deltaGmu()
8398  -0.319 * deltaMz()
8399  -0.351 * deltaMh() );
8400 
8401  } else if (Pol_em == -80. && Pol_ep == 30.){
8402  mu +=
8403  +121273. * CiHbox / LambdaNP2
8404  +6488707. * CiHL1_11 / LambdaNP2
8405  -332950. * CiHe_11 / LambdaNP2
8406  +6488707. * CiHL3_11 / LambdaNP2
8407  -67530.9 * CiHD / LambdaNP2
8408  -408101. * CiHB / LambdaNP2
8409  +1576859. * CiHW / LambdaNP2
8410  -260777. * CiHWB / LambdaNP2
8411  -452746. * CiDHB / LambdaNP2
8412  +796569. * CiDHW / LambdaNP2
8413  -4.231 * DeltaGF()
8414  ;
8415 
8416  // Add modifications due to small variations of the SM parameters
8417  mu += cHSM * ( -2.23 * deltaaMZ()
8418  +4.23 * deltaGmu()
8419  +9.06 * deltaMz()
8420  -0.351 * deltaMh() );
8421 
8422  } else if (Pol_em == 80. && Pol_ep == 0.){
8423  mu +=
8424  +121280. * CiHbox / LambdaNP2
8425  +887632. * CiHL1_11 / LambdaNP2
8426  -6858533. * CiHe_11 / LambdaNP2
8427  +887632. * CiHL3_11 / LambdaNP2
8428  +65606.6 * CiHD / LambdaNP2
8429  +927745. * CiHB / LambdaNP2
8430  +241619. * CiHW / LambdaNP2
8431  +1223535. * CiHWB / LambdaNP2
8432  +894441. * CiDHB / LambdaNP2
8433  +58317. * CiDHW / LambdaNP2
8434  +0.161 * DeltaGF()
8435  ;
8436 
8437  // Add modifications due to small variations of the SM parameters
8438  mu += cHSM * ( +2.163 * deltaaMZ()
8439  -0.163 * deltaGmu()
8440  +0.275 * deltaMz()
8441  -0.351 * deltaMh() );
8442 
8443  } else if (Pol_em == -80. && Pol_ep == 0.){
8444  mu +=
8445  +121268. * CiHbox / LambdaNP2
8446  +6262095. * CiHL1_11 / LambdaNP2
8447  -597046. * CiHe_11 / LambdaNP2
8448  +6262095. * CiHL3_11 / LambdaNP2
8449  -62148.8 * CiHD / LambdaNP2
8450  -353914. * CiHB / LambdaNP2
8451  +1522841. * CiHW / LambdaNP2
8452  -200684. * CiHWB / LambdaNP2
8453  -398214. * CiDHB / LambdaNP2
8454  +766821. * CiDHW / LambdaNP2
8455  -4.054 * DeltaGF()
8456  ;
8457 
8458  // Add modifications due to small variations of the SM parameters
8459  mu += cHSM * ( -2.052 * deltaaMZ()
8460  +4.052 * deltaGmu()
8461  +8.704 * deltaMz()
8462  -0.351 * deltaMh() );
8463 
8464  } else {
8465  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8466  }
8467 
8468  } else if (sqrt_s == 1.0) {
8469 
8470  C1 = -0.0012;
8471 
8472  if (Pol_em == 80. && Pol_ep == -30.){
8473  mu +=
8474  +121236. * CiHbox / LambdaNP2
8475  +2034785. * CiHL1_11 / LambdaNP2
8476  -29195703. * CiHe_11 / LambdaNP2
8477  +2034785. * CiHL3_11 / LambdaNP2
8478  +74612.7 * CiHD / LambdaNP2
8479  +1218284. * CiHB / LambdaNP2
8480  +154779. * CiHW / LambdaNP2
8481  +1507673. * CiHWB / LambdaNP2
8482  +4701988. * CiDHB / LambdaNP2
8483  +239404. * CiDHW / LambdaNP2
8484  +0.458 * DeltaGF()
8485  ;
8486 
8487  // Add modifications due to small variations of the SM parameters
8488  mu += cHSM * ( +2.46 * deltaaMZ()
8489  -0.46 * deltaGmu()
8490  -0.745 * deltaMz()
8491  -0.092 * deltaMh() );
8492 
8493  } else if (Pol_em == -80. && Pol_ep == 30.){
8494  mu +=
8495  +121298. * CiHbox / LambdaNP2
8496  +25954994. * CiHL1_11 / LambdaNP2
8497  -1333713. * CiHe_11 / LambdaNP2
8498  +25954994. * CiHL3_11 / LambdaNP2
8499  -67536.7 * CiHD / LambdaNP2
8500  -499699. * CiHB / LambdaNP2
8501  +1872177. * CiHW / LambdaNP2
8502  -263454. * CiHWB / LambdaNP2
8503  -1999387. * CiDHB / LambdaNP2
8504  +3910434. * CiDHW / LambdaNP2
8505  -4.233 * DeltaGF()
8506  ;
8507 
8508  // Add modifications due to small variations of the SM parameters
8509  mu += cHSM * ( -2.23 * deltaaMZ()
8510  +4.23 * deltaGmu()
8511  +8.633 * deltaMz()
8512  -0.092 * deltaMh() );
8513 
8514  } else if (Pol_em == 80. && Pol_ep == -20.){
8515  mu +=
8516  +121257. * CiHbox / LambdaNP2
8517  +2475072. * CiHL1_11 / LambdaNP2
8518  -28682974. * CiHe_11 / LambdaNP2
8519  +2475072. * CiHL3_11 / LambdaNP2
8520  +72023. * CiHD / LambdaNP2
8521  +1186280. * CiHB / LambdaNP2
8522  +186435. * CiHW / LambdaNP2
8523  +1475072. * CiHWB / LambdaNP2
8524  +4578518. * CiDHB / LambdaNP2
8525  +307070. * CiDHW / LambdaNP2
8526  +0.371 * DeltaGF()
8527  ;
8528 
8529  // Add modifications due to small variations of the SM parameters
8530  mu += cHSM * ( -0.572 * deltaMz()
8531  -0.091 * deltaMh()
8532  +2.375 * deltaaMZ()
8533  -0.377 * deltaGmu() );
8534 
8535  } else if (Pol_em == -80. && Pol_ep == 20.){
8536  mu +=
8537  +121306. * CiHbox / LambdaNP2
8538  +25696973. * CiHL1_11 / LambdaNP2
8539  -1634825. * CiHe_11 / LambdaNP2
8540  +25696973. * CiHL3_11 / LambdaNP2
8541  -65976.8 * CiHD / LambdaNP2
8542  -480973. * CiHB / LambdaNP2
8543  +1853631. * CiHW / LambdaNP2
8544  -244288. * CiHWB / LambdaNP2
8545  -1927204. * CiDHB / LambdaNP2
8546  +3870798. * CiDHW / LambdaNP2
8547  -4.182 * DeltaGF()
8548  ;
8549 
8550  // Add modifications due to small variations of the SM parameters
8551  mu += cHSM * ( +8.536 * deltaMz()
8552  -0.09 * deltaMh()
8553  -2.178 * deltaaMZ()
8554  +4.178 * deltaGmu() );
8555 
8556  } else if (Pol_em == 80. && Pol_ep == 0.){
8557  mu +=
8558  +121307. * CiHbox / LambdaNP2
8559  +3550656. * CiHL1_11 / LambdaNP2
8560  -27432206. * CiHe_11 / LambdaNP2
8561  +3550656. * CiHL3_11 / LambdaNP2
8562  +65607.4 * CiHD / LambdaNP2
8563  +1109435. * CiHB / LambdaNP2
8564  +263679. * CiHW / LambdaNP2
8565  +1395519. * CiHWB / LambdaNP2
8566  +4277336. * CiDHB / LambdaNP2
8567  +472106. * CiDHW / LambdaNP2
8568  +0.159 * DeltaGF()
8569  ;
8570 
8571  // Add modifications due to small variations of the SM parameters
8572  mu += cHSM * ( +2.163 * deltaaMZ()
8573  -0.163 * deltaGmu()
8574  -0.151 * deltaMz()
8575  -0.092 * deltaMh() );
8576 
8577  } else if (Pol_em == -80. && Pol_ep == 0.){
8578  mu +=
8579  +121327. * CiHbox / LambdaNP2
8580  +25048839. * CiHL1_11 / LambdaNP2
8581  -2390358. * CiHe_11 / LambdaNP2
8582  +25048839. * CiHL3_11 / LambdaNP2
8583  -62132.7 * CiHD / LambdaNP2
8584  -434824. * CiHB / LambdaNP2
8585  +1807095. * CiHW / LambdaNP2
8586  -196264. * CiHWB / LambdaNP2
8587  -1746222. * CiDHB / LambdaNP2
8588  +3771341. * CiDHW / LambdaNP2
8589  -4.056 * DeltaGF()
8590  ;
8591 
8592  // Add modifications due to small variations of the SM parameters
8593  mu += cHSM * ( -2.052 * deltaaMZ()
8594  +4.052 * deltaGmu()
8595  +8.278 * deltaMz()
8596  -0.092 * deltaMh() );
8597 
8598  } else {
8599  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8600  }
8601 
8602  } else if (sqrt_s == 1.4) {
8603 
8604  C1 = -0.0011;
8605 
8606  if (Pol_em == 80. && Pol_ep == -30.){
8607  mu +=
8608  +121277. * CiHbox / LambdaNP2
8609  +3988231. * CiHL1_11 / LambdaNP2
8610  -57226150. * CiHe_11 / LambdaNP2
8611  +3988231. * CiHL3_11 / LambdaNP2
8612  +74608.5 * CiHD / LambdaNP2
8613  +1256970. * CiHB / LambdaNP2
8614  +155358. * CiHW / LambdaNP2
8615  +1542655. * CiHWB / LambdaNP2
8616  +9506894. * CiDHB / LambdaNP2
8617  +553431. * CiDHW / LambdaNP2
8618  +0.457 * DeltaGF()
8619  ;
8620 
8621  // Add modifications due to small variations of the SM parameters
8622  mu += cHSM * ( +2.46 * deltaaMZ()
8623  -0.46 * deltaGmu()
8624  -0.828 * deltaMz()
8625  -0.047 * deltaMh() );
8626 
8627  } else if (Pol_em == -80. && Pol_ep == 30.){
8628  mu +=
8629  +121314. * CiHbox / LambdaNP2
8630  +50871646. * CiHL1_11 / LambdaNP2
8631  -2614134. * CiHe_11 / LambdaNP2
8632  +50871646. * CiHL3_11 / LambdaNP2
8633  -67535.5 * CiHD / LambdaNP2
8634  -516385. * CiHB / LambdaNP2
8635  +1928805. * CiHW / LambdaNP2
8636  -264072. * CiHWB / LambdaNP2
8637  -3989947. * CiDHB / LambdaNP2
8638  +7948308. * CiDHW / LambdaNP2
8639  -4.233 * DeltaGF()
8640  ;
8641 
8642  // Add modifications due to small variations of the SM parameters
8643  mu += cHSM * ( -2.23 * deltaaMZ()
8644  +4.23 * deltaGmu()
8645  +8.55 * deltaMz()
8646  -0.047 * deltaMh() );
8647 
8648  } else if (Pol_em == 80. && Pol_ep == 0.){
8649  mu +=
8650  +121250. * CiHbox / LambdaNP2
8651  +6958750. * CiHL1_11 / LambdaNP2
8652  -53762500. * CiHe_11 / LambdaNP2
8653  +6958750. * CiHL3_11 / LambdaNP2
8654  +65589.3 * CiHD / LambdaNP2
8655  +1144464. * CiHB / LambdaNP2
8656  +267732. * CiHW / LambdaNP2
8657  +1428214. * CiHWB / LambdaNP2
8658  +8650536. * CiDHB / LambdaNP2
8659  +1021964. * CiDHW / LambdaNP2
8660  +0.16 * DeltaGF()
8661  ;
8662 
8663  // Add modifications due to small variations of the SM parameters
8664  mu += cHSM * ( +2.163 * deltaaMZ()
8665  -0.163 * deltaGmu()
8666  -0.234 * deltaMz()
8667  -0.047 * deltaMh() );
8668 
8669  } else if (Pol_em == -80. && Pol_ep == 0.){
8670  mu +=
8671  +121278. * CiHbox / LambdaNP2
8672  +49094486. * CiHL1_11 / LambdaNP2
8673  -4685522. * CiHe_11 / LambdaNP2
8674  +49094486. * CiHL3_11 / LambdaNP2
8675  -62150.9 * CiHD / LambdaNP2
8676  -450090. * CiHB / LambdaNP2
8677  +1861602. * CiHW / LambdaNP2
8678  -195621. * CiHWB / LambdaNP2
8679  -3478338. * CiDHB / LambdaNP2
8680  +7668095. * CiDHW / LambdaNP2
8681  -4.055 * DeltaGF()
8682  ;
8683 
8684  // Add modifications due to small variations of the SM parameters
8685  mu += cHSM * ( -2.052 * deltaaMZ()
8686  +4.052 * deltaGmu()
8687  +8.195 * deltaMz()
8688  -0.047 * deltaMh() );
8689 
8690  } else {
8691  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8692  }
8693 
8694  } else if (sqrt_s == 1.5) {
8695 
8696  C1 = -0.0011;// Use the same as 1400 GeV
8697 
8698  if (Pol_em == 80. && Pol_ep == -30.){
8699  mu +=
8700  +121268. * CiHbox / LambdaNP2
8701  +4578315. * CiHL1_11 / LambdaNP2
8702  -65691823. * CiHe_11 / LambdaNP2
8703  +4578315. * CiHL3_11 / LambdaNP2
8704  +74595.2 * CiHD / LambdaNP2
8705  +1262261. * CiHB / LambdaNP2
8706  +155435. * CiHW / LambdaNP2
8707  +1547379. * CiHWB / LambdaNP2
8708  +10961322. * CiDHB / LambdaNP2
8709  +649157. * CiDHW / LambdaNP2
8710  +0.457 * DeltaGF()
8711  ;
8712 
8713  // Add modifications due to small variations of the SM parameters
8714  mu += cHSM * ( +2.46 * deltaaMZ()
8715  -0.46 * deltaGmu()
8716  -0.84 * deltaMz()
8717  -0.041 * deltaMh() );
8718 
8719  } else if (Pol_em == -80. && Pol_ep == 30.){
8720  mu +=
8721  +121277. * CiHbox / LambdaNP2
8722  +58398883. * CiHL1_11 / LambdaNP2
8723  -3000385. * CiHe_11 / LambdaNP2
8724  +58398883. * CiHL3_11 / LambdaNP2
8725  -67535.8 * CiHD / LambdaNP2
8726  -518798. * CiHB / LambdaNP2
8727  +1936613. * CiHW / LambdaNP2
8728  -264171. * CiHWB / LambdaNP2
8729  -4590136. * CiDHB / LambdaNP2
8730  +9169803. * CiDHW / LambdaNP2
8731  -4.233 * DeltaGF()
8732  ;
8733 
8734  // Add modifications due to small variations of the SM parameters
8735  mu += cHSM * ( -2.23 * deltaaMZ()
8736  +4.23 * deltaGmu()
8737  +8.539 * deltaMz()
8738  -0.041 * deltaMh() );
8739 
8740  } else if (Pol_em == 80. && Pol_ep == 0.){
8741  mu +=
8742  +121289. * CiHbox / LambdaNP2
8743  +7988570. * CiHL1_11 / LambdaNP2
8744  -61718691. * CiHe_11 / LambdaNP2
8745  +7988570. * CiHL3_11 / LambdaNP2
8746  +65599. * CiHD / LambdaNP2
8747  +1149083. * CiHB / LambdaNP2
8748  +268317. * CiHW / LambdaNP2
8749  +1432777. * CiHWB / LambdaNP2
8750  +9972576. * CiDHB / LambdaNP2
8751  +1188554. * CiDHW / LambdaNP2
8752  +0.16 * DeltaGF()
8753  ;
8754 
8755  // Add modifications due to small variations of the SM parameters
8756  mu += cHSM * ( +2.163 * deltaaMZ()
8757  -0.163 * deltaGmu()
8758  -0.246 * deltaMz()
8759  -0.041 * deltaMh() );
8760 
8761  } else if (Pol_em == -80. && Pol_ep == 0.){
8762  mu +=
8763  +121259. * CiHbox / LambdaNP2
8764  +56356946. * CiHL1_11 / LambdaNP2
8765  -5378233. * CiHe_11 / LambdaNP2
8766  +56356946. * CiHL3_11 / LambdaNP2
8767  -62168.7 * CiHD / LambdaNP2
8768  -452149. * CiHB / LambdaNP2
8769  +1869136. * CiHW / LambdaNP2
8770  -195562. * CiHWB / LambdaNP2
8771  -4000306. * CiDHB / LambdaNP2
8772  +8846432. * CiDHW / LambdaNP2
8773  -4.055 * DeltaGF()
8774  ;
8775 
8776  // Add modifications due to small variations of the SM parameters
8777  mu += cHSM * ( -2.052 * deltaaMZ()
8778  +4.052 * deltaGmu()
8779  +8.183 * deltaMz()
8780  -0.041 * deltaMh() );
8781 
8782  } else {
8783  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8784  }
8785 
8786  } else if (sqrt_s == 3.0) {
8787 
8788  C1 = -0.00054;
8789 
8790  if (Pol_em == 80. && Pol_ep == -30.){
8791  mu +=
8792  +121320. * CiHbox / LambdaNP2
8793  +18314161. * CiHL1_11 / LambdaNP2
8794  -262773345. * CiHe_11 / LambdaNP2
8795  +18314161. * CiHL3_11 / LambdaNP2
8796  +74663.6 * CiHD / LambdaNP2
8797  +1289569. * CiHB / LambdaNP2
8798  +155612. * CiHW / LambdaNP2
8799  +1572580. * CiHWB / LambdaNP2
8800  +44806408. * CiDHB / LambdaNP2
8801  +2877519. * CiDHW / LambdaNP2
8802  +0.456 * DeltaGF()
8803  ;
8804 
8805  // Add modifications due to small variations of the SM parameters
8806  mu += cHSM * ( +2.46 * deltaaMZ()
8807  -0.46 * deltaGmu()
8808  -0.899 * deltaMz()
8809  -0.01 * deltaMh() );
8810 
8811  } else if (Pol_em == -80. && Pol_ep == 30.){
8812  mu +=
8813  +121305. * CiHbox / LambdaNP2
8814  +233598342. * CiHL1_11 / LambdaNP2
8815  -12002450. * CiHe_11 / LambdaNP2
8816  +233598342. * CiHL3_11 / LambdaNP2
8817  -67507.7 * CiHD / LambdaNP2
8818  -531387. * CiHB / LambdaNP2
8819  +1976750. * CiHW / LambdaNP2
8820  -264661. * CiHWB / LambdaNP2
8821  -18587969. * CiDHB / LambdaNP2
8822  +37618569. * CiDHW / LambdaNP2
8823  -4.233 * DeltaGF()
8824  ;
8825 
8826  // Add modifications due to small variations of the SM parameters
8827  mu += cHSM * ( -2.23 * deltaaMZ()
8828  +4.23 * deltaGmu()
8829  +8.48 * deltaMz()
8830  -0.01 * deltaMh() );
8831 
8832  } else if (Pol_em == 80. && Pol_ep == 0.){
8833  mu +=
8834  +121225. * CiHbox / LambdaNP2
8835  +31953446. * CiHL1_11 / LambdaNP2
8836  -246870182. * CiHe_11 / LambdaNP2
8837  +31953446. * CiHL3_11 / LambdaNP2
8838  +65576.5 * CiHD / LambdaNP2
8839  +1173703. * CiHB / LambdaNP2
8840  +270983. * CiHW / LambdaNP2
8841  +1456032. * CiHWB / LambdaNP2
8842  +40783748. * CiDHB / LambdaNP2
8843  +5077924. * CiDHW / LambdaNP2
8844  +0.16 * DeltaGF()
8845  ;
8846 
8847  // Add modifications due to small variations of the SM parameters
8848  mu += cHSM * ( +2.163 * deltaaMZ()
8849  -0.163 * deltaGmu()
8850  -0.305 * deltaMz()
8851  -0.01 * deltaMh() );
8852 
8853  } else if (Pol_em == -80. && Pol_ep == 0.){
8854  mu +=
8855  +121248. * CiHbox / LambdaNP2
8856  +225427310. * CiHL1_11 / LambdaNP2
8857  -21505526. * CiHe_11 / LambdaNP2
8858  +225427310. * CiHL3_11 / LambdaNP2
8859  -62193.4 * CiHD / LambdaNP2
8860  -463403. * CiHB / LambdaNP2
8861  +1907593. * CiHW / LambdaNP2
8862  -195017. * CiHWB / LambdaNP2
8863  -16188019. * CiDHB / LambdaNP2
8864  +36299719. * CiDHW / LambdaNP2
8865  -4.054 * DeltaGF()
8866  ;
8867 
8868  // Add modifications due to small variations of the SM parameters
8869  mu += cHSM * ( -2.052 * deltaaMZ()
8870  +4.052 * deltaGmu()
8871  +8.124 * deltaMz()
8872  -0.01 * deltaMh() );
8873 
8874  } else {
8875  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8876  }
8877 
8878  } else
8879  throw std::runtime_error("Bad argument in NPSMEFTd6::mueeZHPol()");
8880 
8881  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
8882  mu += eeeZHint + eeeZHpar;
8883 
8884 // Linear contribution from Higgs self-coupling
8885  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
8886 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
8888 
8889  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
8890 
8891  return mu;
8892 }

◆ mueeZllH()

double NPSMEFTd6::mueeZllH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\)

Reimplemented from NPbase.

Definition at line 7865 of file NPSMEFTd6.cpp.

7866 {
7867 
7868 // The signal strength eeZH
7869  double mu = mueeZH(sqrt_s);
7870 
7871 // The (relative) linear correction to the Z>ll BR
7872  double deltaBRratio;
7873 
7874  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
7875  + deltaGamma_Zf(leptons[MU]);
7876 
7877  deltaBRratio = deltaBRratio /
7879 
7880  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
7881 
7882  return mu + deltaBRratio;
7883 }

◆ mueeZllHPol()

double NPSMEFTd6::mueeZllHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\)

Reimplemented from NPbase.

Definition at line 8894 of file NPSMEFTd6.cpp.

8895 {
8896 
8897 // The signal strength eeZH
8898  double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
8899 
8900 // The (relative) linear correction to the Z>ll BR
8901  double deltaBRratio;
8902 
8903  deltaBRratio = deltaGamma_Zf(leptons[ELECTRON])
8904  + deltaGamma_Zf(leptons[MU]);
8905 
8906  deltaBRratio = deltaBRratio /
8908 
8909  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
8910 
8911  return mu + deltaBRratio;
8912 }

◆ mueeZqqH()

double NPSMEFTd6::mueeZqqH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{eeZH, Z \to q \bar{q}}\)

Reimplemented from NPbase.

Definition at line 7885 of file NPSMEFTd6.cpp.

7886 {
7887 
7888 // The signal strength eeZH
7889  double mu = mueeZH(sqrt_s);
7890 
7891 // The (relative) linear correction to the Z>qq BR
7892  double deltaBRratio;
7893 
7894  deltaBRratio = deltaGamma_Zf(quarks[UP])
7899 
7900  deltaBRratio = deltaBRratio /
7903  + trueSM.GammaZ(quarks[BOTTOM]));
7904 
7905  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
7906 
7907  return mu + deltaBRratio;
7908 }

◆ mueeZqqHPol()

double NPSMEFTd6::mueeZqqHPol ( const double  sqrt_s,
const double  Pol_em,
const double  Pol_ep 
) const
virtual

The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively
Returns
\(\mu_{eeZH, Z \to q \bar{q}}\)

Reimplemented from NPbase.

Definition at line 8914 of file NPSMEFTd6.cpp.

8915 {
8916 
8917 // The signal strength eeZH
8918  double mu = mueeZHPol(sqrt_s, Pol_em, Pol_ep);
8919 
8920 // The (relative) linear correction to the Z>qq BR
8921  double deltaBRratio;
8922 
8923  deltaBRratio = deltaGamma_Zf(quarks[UP])
8928 
8929  deltaBRratio = deltaBRratio /
8932  + trueSM.GammaZ(quarks[BOTTOM]));
8933 
8934  deltaBRratio = deltaBRratio - deltaGamma_Z() / trueSM.Gamma_Z();
8935 
8936  return mu + deltaBRratio;
8937 }

◆ muepWBF()

double NPSMEFTd6::muepWBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{epWBF}\)

Reimplemented from NPbase.

Definition at line 6982 of file NPSMEFTd6.cpp.

6983 {
6984  double mu = 1.0;
6985 
6986  if (sqrt_s == 1.3) {
6987 
6988  mu +=
6989  +121790. * CiHbox / LambdaNP2
6990  -161604. * CiHL3_11 / LambdaNP2
6991  -161282. * CiHQ3_11 / LambdaNP2
6992  -203141. * CiHD / LambdaNP2
6993  -88171.6 * CiHW / LambdaNP2
6994  -377218. * CiHWB / LambdaNP2
6995  -37738.9 * CiDHW / LambdaNP2
6996  -4.676 * DeltaGF()
6997  -4.916 * deltaMwd6()
6998  ;
6999 
7000 // if (FlagQuadraticTerms) {
7001  //Add contributions that are quadratic in the effective coefficients
7002 
7003 // }
7004 
7005  } else if (sqrt_s == 1.8) {
7006 
7007  mu +=
7008  +121867. * CiHbox / LambdaNP2
7009  -182643. * CiHL3_11 / LambdaNP2
7010  -181961. * CiHQ3_11 / LambdaNP2
7011  -202400. * CiHD / LambdaNP2
7012  -78295.8 * CiHW / LambdaNP2
7013  -377193. * CiHWB / LambdaNP2
7014  -45757.3 * CiDHW / LambdaNP2
7015  -4.672 * DeltaGF()
7016  -4.637 * deltaMwd6()
7017  ;
7018 
7019 // if (FlagQuadraticTerms) {
7020  //Add contributions that are quadratic in the effective coefficients
7021 
7022 // }
7023 
7024  } else if (sqrt_s == 3.5) {
7025 
7026  mu +=
7027  +121250. * CiHbox / LambdaNP2
7028  -216885. * CiHL3_11 / LambdaNP2
7029  -218544. * CiHQ3_11 / LambdaNP2
7030  -202390. * CiHD / LambdaNP2
7031  -64783.2 * CiHW / LambdaNP2
7032  -377727. * CiHWB / LambdaNP2
7033  -60431.2 * CiDHW / LambdaNP2
7034  -4.688 * DeltaGF()
7035  -4.573 * deltaMwd6()
7036  ;
7037 
7038 // if (FlagQuadraticTerms) {
7039  //Add contributions that are quadratic in the effective coefficients
7040 
7041 // }
7042 
7043  } else if (sqrt_s == 5.0) {
7044 
7045  mu +=
7046  +119662. * CiHbox / LambdaNP2
7047  -237868. * CiHL3_11 / LambdaNP2
7048  -236470. * CiHQ3_11 / LambdaNP2
7049  -203294. * CiHD / LambdaNP2
7050  -60911. * CiHW / LambdaNP2
7051  -378045. * CiHWB / LambdaNP2
7052  -67483.7 * CiDHW / LambdaNP2
7053  -4.667 * DeltaGF()
7054  -4.437 * deltaMwd6()
7055  ;
7056 
7057 // if (FlagQuadraticTerms) {
7058  //Add contributions that are quadratic in the effective coefficients
7059 
7060 // }
7061 
7062  } else
7063  throw std::runtime_error("Bad argument in NPSMEFTd6::muepWBF()");
7064 
7065  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7066  mu += eepWBFint + eepWBFpar;
7067 
7068  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7069 
7070  return mu;
7071 }

◆ muepZBF()

double NPSMEFTd6::muepZBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{epZBF}\)

Reimplemented from NPbase.

Definition at line 7073 of file NPSMEFTd6.cpp.

7074 {
7075  double mu = 1.0;
7076 
7077  if (sqrt_s == 1.3) {
7078 
7079  mu +=
7080  +121280. * CiHbox / LambdaNP2
7081  -152367. * CiHL1_11 / LambdaNP2
7082  +32200. * CiHQ1_11 / LambdaNP2
7083  +124934. * CiHe_11 / LambdaNP2
7084  -42209.5 * CiHu_11 / LambdaNP2
7085  +12445.7 * CiHd_11 / LambdaNP2
7086  -152367. * CiHL3_11 / LambdaNP2
7087  -165343. * CiHQ3_11 / LambdaNP2
7088  -173922. * CiHD / LambdaNP2
7089  -34636.2 * CiHB / LambdaNP2
7090  -121438. * CiHW / LambdaNP2
7091  -74939.1 * CiHWB / LambdaNP2
7092  -5454.93 * CiDHB / LambdaNP2
7093  -39349.6 * CiDHW / LambdaNP2
7094  -3.719 * DeltaGF()
7095  ;
7096 
7097 // if (FlagQuadraticTerms) {
7098  //Add contributions that are quadratic in the effective coefficients
7099 
7100 // }
7101 
7102  } else if (sqrt_s == 1.8) {
7103 
7104  mu +=
7105  +120218. * CiHbox / LambdaNP2
7106  -173566. * CiHL1_11 / LambdaNP2
7107  +26307.1 * CiHQ1_11 / LambdaNP2
7108  +142600. * CiHe_11 / LambdaNP2
7109  -47449. * CiHu_11 / LambdaNP2
7110  +14356.2 * CiHd_11 / LambdaNP2
7111  -173566. * CiHL3_11 / LambdaNP2
7112  -188606. * CiHQ3_11 / LambdaNP2
7113  -174301. * CiHD / LambdaNP2
7114  -19800. * CiHB / LambdaNP2
7115  -103254. * CiHW / LambdaNP2
7116  -89049.2 * CiHWB / LambdaNP2
7117  -8304.85 * CiDHB / LambdaNP2
7118  -48942.9 * CiDHW / LambdaNP2
7119  -3.714 * DeltaGF()
7120  ;
7121 
7122 // if (FlagQuadraticTerms) {
7123  //Add contributions that are quadratic in the effective coefficients
7124 
7125 // }
7126 
7127  } else if (sqrt_s == 3.5) {
7128 
7129  mu +=
7130  +123119. * CiHbox / LambdaNP2
7131  -206981. * CiHL1_11 / LambdaNP2
7132  +18620.9 * CiHQ1_11 / LambdaNP2
7133  +177706. * CiHe_11 / LambdaNP2
7134  -53822. * CiHu_11 / LambdaNP2
7135  +20491.5 * CiHd_11 / LambdaNP2
7136  -206981. * CiHL3_11 / LambdaNP2
7137  -227549. * CiHQ3_11 / LambdaNP2
7138  -172298. * CiHD / LambdaNP2
7139  -6887.17 * CiHB / LambdaNP2
7140  -79245. * CiHW / LambdaNP2
7141  -103223. * CiHWB / LambdaNP2
7142  -9863.11 * CiDHB / LambdaNP2
7143  -61304.3 * CiDHW / LambdaNP2
7144  -3.721 * DeltaGF()
7145  ;
7146 
7147 // if (FlagQuadraticTerms) {
7148  //Add contributions that are quadratic in the effective coefficients
7149 
7150 // }
7151 
7152  } else if (sqrt_s == 5.0) {
7153 
7154  mu +=
7155  +121709. * CiHbox / LambdaNP2
7156  -225267. * CiHL1_11 / LambdaNP2
7157  +13471.8 * CiHQ1_11 / LambdaNP2
7158  +193542. * CiHe_11 / LambdaNP2
7159  -57640.9 * CiHu_11 / LambdaNP2
7160  +22573. * CiHd_11 / LambdaNP2
7161  -225267. * CiHL3_11 / LambdaNP2
7162  -247738. * CiHQ3_11 / LambdaNP2
7163  -172768. * CiHD / LambdaNP2
7164  -4524.89 * CiHB / LambdaNP2
7165  -71935.4 * CiHW / LambdaNP2
7166  -104998. * CiHWB / LambdaNP2
7167  -11877.8 * CiDHB / LambdaNP2
7168  -69467.3 * CiDHW / LambdaNP2
7169  -3.71 * DeltaGF()
7170  ;
7171 
7172 // if (FlagQuadraticTerms) {
7173  //Add contributions that are quadratic in the effective coefficients
7174 
7175 // }
7176 
7177  } else
7178  throw std::runtime_error("Bad argument in NPSMEFTd6::muepZBF()");
7179 
7180  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7181  mu += eepZBFint + eepZBFpar;
7182 
7183  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7184 
7185  return mu;
7186 }

◆ muggH()

double NPSMEFTd6::muggH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH}\)

Reimplemented from NPbase.

Definition at line 3623 of file NPSMEFTd6.cpp.

3624 {
3625 
3626  double C1 = 0.0066; //It seems to be independent of energy
3627 
3628  double m_t = mtpole;
3629  //doulbe m_t = quarks[TOP].getMass();
3630  double m_b = quarks[BOTTOM].getMass();
3631  double m_c = quarks[CHARM].getMass();
3632 
3633  /* L_eff_SM = (G_eff_t_SM + G_eff_b_SM)*hGG */
3634  gslpp::complex G_eff_t_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_t * m_t / mHl / mHl);
3635  gslpp::complex G_eff_b_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_b * m_b / mHl / mHl);
3636  gslpp::complex G_eff_c_SM = AlsMz / 16.0 / M_PI / v() * AH_f(4.0 * m_c * m_c / mHl / mHl);
3637  gslpp::complex G_eff_SM = G_eff_t_SM + G_eff_b_SM + G_eff_c_SM;
3638 
3639  //double sigma_tt_SM = trueSM.computeSigmaggH_tt(sqrt_s);
3640  //double sigma_bb_SM = trueSM.computeSigmaggH_bb(sqrt_s);
3641  //double sigma_tb_SM = trueSM.computeSigmaggH_tb(sqrt_s);
3642  //gslpp::complex tmp = (2.0 * dKappa_t * sigma_tt_SM
3643  // + 2.0 * dKappa_b * sigma_bb_SM
3644  // + (dKappa_t + dKappa_b) * sigma_tb_SM)
3645  // / (sigma_tt_SM + sigma_bb_SM + sigma_tb_SM);
3646 
3647  gslpp::complex dKappa_t = cLHd6 * deltaG_hff(quarks[TOP]) / (-m_t / v());
3648  gslpp::complex dKappa_b = cLHd6 * deltaG_hff(quarks[BOTTOM]) / (-m_b / v());
3649  gslpp::complex dKappa_c = cLHd6 * deltaG_hff(quarks[CHARM]) / (-m_c / v());
3650 
3651  gslpp::complex tmpHG = CHG / v() * v2_over_LambdaNP2 / G_eff_SM;
3652  gslpp::complex tmpt = G_eff_t_SM * dKappa_t / G_eff_SM;
3653  gslpp::complex tmpb = G_eff_b_SM * dKappa_b / G_eff_SM;
3654  gslpp::complex tmpc = G_eff_c_SM * dKappa_c / G_eff_SM;
3655 
3656  double mu = (1.0 + 2.0 * ( tmpt.real() + tmpb.real() + tmpc.real() + tmpHG.real() ) );
3657 
3658 // Linear contribution from Higgs self-coupling
3659  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3660 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3662 
3663  if (FlagQuadraticTerms) {
3664  //Add contributions that are quadratic in the effective coefficients
3665  gslpp::complex tmp2 = tmpt +tmpb +tmpc + tmpHG;
3666 
3667  mu += tmp2.abs2();
3668 
3669  }
3670 
3671  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3672  mu += eggFint + eggFpar;
3673 
3674  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3675 
3676  return mu;
3677 }

◆ muggHbb()

double NPSMEFTd6::muggHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,bb}\)

Reimplemented from NPbase.

Definition at line 13146 of file NPSMEFTd6.cpp.

13147 {
13148  return muggH(sqrt_s) * BrHbbRatio();
13149 
13150 }

◆ muggHgaga()

double NPSMEFTd6::muggHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12858 of file NPSMEFTd6.cpp.

12859 {
12860  return muggH(sqrt_s) * BrHgagaRatio();
12861 
12862 }

◆ muggHH()

double NPSMEFTd6::muggHH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggHH}\)

Reimplemented from NPbase.

Definition at line 3679 of file NPSMEFTd6.cpp.

3680 {
3681  double mu = 1.0;
3682  double A1HH = 0.0, A2HH = 0.0, A3HH = 0.0, A4HH = 0.0, A5HH = 0.0;
3683  double A6HH = 0.0, A7HH = 0.0, A8HH = 0.0, A9HH = 0.0, A10HH = 0.0;
3684  double A11HH = 0.0, A12HH = 0.0, A13HH = 0.0, A14HH = 0.0, A15HH = 0.0;
3685  double ct,c2t,c3,cg,c2g;
3686 
3687  if (sqrt_s == 14.0) {
3688 
3689  // From the cut-based analysis. Table IV
3690 
3691  A1HH = 1.70;
3692  A2HH = 10.7;
3693  A3HH = 0.117;
3694  A4HH = 6.11;
3695  A5HH = 217.0;
3696  A6HH = -7.56;
3697  A7HH = -0.819;
3698  A8HH = 1.95;
3699  A9HH = 10.90;
3700  A10HH = 51.6;
3701  A11HH = -3.86;
3702  A12HH = -12.5;
3703  A13HH = 1.46;
3704  A14HH = 5.49;
3705  A15HH = 58.4;
3706 
3707  } else if (sqrt_s == 100.0) {
3708 
3709  // From the cut-based analysis. Table IV
3710 
3711  A1HH = 1.59;
3712  A2HH = 12.8;
3713  A3HH = 0.090;
3714  A4HH = 5.2;
3715  A5HH = 358.0;
3716  A6HH = -7.66;
3717  A7HH = -0.681;
3718  A8HH = 1.83;
3719  A9HH = 9.25;
3720  A10HH = 51.2;
3721  A11HH = -2.61;
3722  A12HH = -7.35;
3723  A13HH = 1.03;
3724  A14HH = 4.65;
3725  A15HH = 65.5;
3726 
3727  } else
3728  throw std::runtime_error("Bad argument in NPSMEFTd6::muggHH()");
3729 
3730  ct= 1.0 - 0.5 * DeltaGF() + delta_h - v() * CiuH_33r * v2_over_LambdaNP2 / sqrt(2.0)/ mtpole;
3731  c2t = delta_h - 3.0 *v() * CiuH_33r * v2_over_LambdaNP2 / 2.0 /sqrt(2.0)/ mtpole;
3732  c3 = 1.0 + deltaG_hhhRatio();
3733  cg = M_PI * CHG * v2_over_LambdaNP2 / AlsMz;
3734  c2g = cg;
3735 
3736 // In the SM the Eq. returns 0.999. Fix that small offset by adding 0.0010
3737  mu = 0.0010 + A1HH*ct*ct*ct*ct +
3738  A2HH*c2t*c2t +
3739  A3HH*ct*ct*c3*c3 +
3740  A4HH*cg*cg*c3*c3 +
3741  A5HH*c2g*c2g +
3742  A6HH*c2t*ct*ct +
3743  A7HH*ct*ct*ct*c3 +
3744  A8HH*c2t*ct*c3 +
3745  A9HH*c2t*cg*c3 +
3746  A10HH*c2t*c2g +
3747  A11HH*ct*ct*cg*c3 +
3748  A12HH*ct*ct*c2g +
3749  A13HH*ct*c3*c3*cg +
3750  A14HH*ct*c3*c2g +
3751  A15HH*cg*c3*c2g;
3752 
3753  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3754 
3755  return mu;
3756 }

◆ muggHmumu()

double NPSMEFTd6::muggHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13074 of file NPSMEFTd6.cpp.

13075 {
13076  return muggH(sqrt_s) * BrHmumuRatio();
13077 
13078 }

◆ muggHpttH()

double NPSMEFTd6::muggHpttH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH+ttH}\)

Reimplemented from NPbase.

Definition at line 9315 of file NPSMEFTd6.cpp.

9316 {
9317  double sigmaggH_SM = computeSigmaggH(sqrt_s);
9318  double sigmattH_SM = computeSigmattH(sqrt_s);
9319  double sigmaggH = muggH(sqrt_s) * sigmaggH_SM;
9320  double sigmattH = muttH(sqrt_s) * sigmattH_SM;
9321 
9322  double mu = ((sigmaggH + sigmattH) / (sigmaggH_SM + sigmattH_SM));
9323 
9324  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9325 
9326  return mu;
9327 }

◆ muggHtautau()

double NPSMEFTd6::muggHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13110 of file NPSMEFTd6.cpp.

13111 {
13112  return muggH(sqrt_s) * BrHtautauRatio();
13113 
13114 }

◆ muggHWW()

double NPSMEFTd6::muggHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW}\)

Reimplemented from NPbase.

Definition at line 13002 of file NPSMEFTd6.cpp.

13003 {
13004  return muggH(sqrt_s) * BrHWWRatio();
13005 
13006 }

◆ muggHWW2l2v()

double NPSMEFTd6::muggHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13038 of file NPSMEFTd6.cpp.

13039 {
13040  return muggH(sqrt_s) * BrHWW2l2vRatio();
13041 
13042 }

◆ muggHZga()

double NPSMEFTd6::muggHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12894 of file NPSMEFTd6.cpp.

12895 {
12896  return muggH(sqrt_s) * BrHZgaRatio();
12897 
12898 }

◆ muggHZZ()

double NPSMEFTd6::muggHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12930 of file NPSMEFTd6.cpp.

12931 {
12932  return muggH(sqrt_s) * BrHZZRatio();
12933 
12934 }

◆ muggHZZ4l()

double NPSMEFTd6::muggHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12966 of file NPSMEFTd6.cpp.

12967 {
12968  return muggH(sqrt_s) * BrHZZ4lRatio();
12969 
12970 }

◆ mummH()

double NPSMEFTd6::mummH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{\mu\mu H}\)

Reimplemented from NPbase.

Definition at line 10182 of file NPSMEFTd6.cpp.

10183 {
10184  double mu = 1.0;
10185 
10186  double dymu = deltaG_hff(leptons[MU]).real();
10187  double ymuSM = -(leptons[MU].getMass()) / v();
10188 
10189 // The ratio at all energies is given by a scaling of the muon Yukawa.
10190  mu = 1.0 + 2.0 * dymu/ymuSM ;
10191 
10192  if (FlagQuadraticTerms) {
10193  //Add contributions that are quadratic in the effective coefficients
10194  mu += dymu*dymu/ymuSM/ymuSM;
10195  }
10196 
10197  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
10198 
10199  return mu;
10200 }

◆ mupTVppWZ()

double NPSMEFTd6::mupTVppWZ ( const double  sqrt_s,
const double  pTV1,
const double  pTV2 
) const
virtual

The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class.

Returns
\(N_{ev}^{p_{TV}}/N_{ev,SM}^{p_{TV}}\)

Reimplemented from NPbase.

Definition at line 14935 of file NPSMEFTd6.cpp.

14936 {
14937  double mu = 1.0;
14938 
14939  double cHWp = 0.0;
14940 
14941  // In the Warsaw basis the contact interactions are generated only by CiHQ3 but
14942  // in the modified basis ODHW also contribute
14943  // Master Equations below are for cHWp = Ci/Lambda^2 in units of TeV^{-2},
14944  // but LambdaNP is in GeV. Add conversion factor.
14945 
14946  cHWp = 4.0 * (sW2_tree/eeMz2) * (CiHQ3_11 + (g2_tree/4.0) * CiDHW) * 1000000.0 / LambdaNP2;
14947 
14948 // Bin dependences assuming cutoff of the EFT at 5 TeV
14949 // Normalize to the total number of events to remove the dependence on Lumi
14950 // (Numbers correspond to 3/ab)
14951  if (sqrt_s == 14.0) {
14952 
14953  if (pTV1 == 100.){
14954  mu += (558.0 * cHWp + 56.8 * cHWp * cHWp) / 3450.0;
14955 
14956  } else if (pTV1 == 150.){
14957  mu += (410.0 * cHWp + 17.64 * cHWp * cHWp) / 2690.0;
14958 
14959  } else if (pTV1 == 220.){
14960  mu += (266.0 * cHWp + 45.6 * cHWp * cHWp) / 925.0;
14961 
14962  } else if (pTV1 == 300.){
14963  mu += (304.0 * cHWp + 108.0 * cHWp * cHWp) / 563.0;
14964 
14965  } else if (pTV1 == 500.){
14966  mu += (114.40 * cHWp + 96.8 * cHWp * cHWp) / 85.1 ;
14967 
14968  } else if (pTV1 == 750.){
14969  mu += (46.20 * cHWp + 86.8 * cHWp * cHWp) / 14.9;
14970 
14971  } else {
14972  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
14973  }
14974 
14975  } else if (sqrt_s == 27.0) {
14976 
14977  if (pTV1 == 150.){
14978  mu += (824.0 * cHWp + 71.6 * cHWp * cHWp) / 5370.0;
14979 
14980  } else if (pTV1 == 220.){
14981  mu += (510.0 * cHWp + 75.2 * cHWp * cHWp) / 2210.0;
14982 
14983  } else if (pTV1 == 300.){
14984  mu += (808.0 * cHWp + 268.4 * cHWp * cHWp) / 1610.0;
14985 
14986  } else if (pTV1 == 500.){
14987  mu += (374.0 * cHWp + 308.0 * cHWp * cHWp) / 331.0;
14988 
14989  } else if (pTV1 == 750.){
14990  mu += (216.0 * cHWp + 420.0 * cHWp * cHWp) / 85.9;
14991 
14992  } else if (pTV1 == 1200.){
14993  mu += (78.2 * cHWp + 325.2 * cHWp * cHWp) / 10.0;
14994 
14995  } else {
14996  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
14997  }
14998 
14999  } else if (sqrt_s == 100.0) {
15000 
15001  if (pTV1 == 220.){
15002  mu += (2000.0 * cHWp + 368.4 * cHWp * cHWp) / 8030.0;
15003 
15004  } else if (pTV1 == 300.){
15005  mu += (2780.0 * cHWp + 1000.0 * cHWp * cHWp) / 7270.0;
15006 
15007  } else if (pTV1 == 500.){
15008  mu += (1544.0 * cHWp + 1428.0 * cHWp * cHWp) / 2000.0;
15009 
15010  } else if (pTV1 == 750.){
15011  mu += (1256.0 * cHWp + 2668.0 * cHWp * cHWp) / 717.0;
15012 
15013  } else if (pTV1 == 1200.){
15014  mu += (678.0 * cHWp + 3400.0 * cHWp * cHWp) / 142.0;
15015 
15016  } else if (pTV1 == 1800.){
15017  mu += (234.0 * cHWp + 2540.0 * cHWp * cHWp) / 27.5;
15018 
15019  } else {
15020  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
15021  }
15022 
15023  } else
15024  throw std::runtime_error("Bad argument in NPSMEFTd6::mupTVppWZ()");
15025 
15026  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
15027 
15028  return mu;
15029 
15030 }

◆ mutHq()

double NPSMEFTd6::mutHq ( const double  sqrt_s) const
virtual

The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{tHq}\)

Reimplemented from NPbase.

Definition at line 9220 of file NPSMEFTd6.cpp.

9221 {
9222  double mu = 1.0;
9223 
9224  double C1 = 0.0;
9225 
9226  if (sqrt_s == 7.0) {
9227 
9228  C1 = 0.0;
9229 
9230  mu += 0.0;
9231 
9232  if (FlagQuadraticTerms) {
9233  //Add contributions that are quadratic in the effective coefficients
9234  mu += 0.0;
9235 
9236  }
9237 
9238  } else if (sqrt_s == 8.0) {
9239 
9240  C1 = 0.0;
9241 
9242  mu += 0.0;
9243 
9244  if (FlagQuadraticTerms) {
9245  //Add contributions that are quadratic in the effective coefficients
9246  mu += 0.0;
9247 
9248  }
9249 
9250  } else if (sqrt_s == 13.0) {
9251 
9252  C1 = 0.0;
9253 
9254  mu += 0.0;
9255 
9256  if (FlagQuadraticTerms) {
9257  //Add contributions that are quadratic in the effective coefficients
9258  mu += 0.0;
9259 
9260  }
9261 
9262  } else if (sqrt_s == 14.0) {
9263 
9264  C1 = 0.0;
9265 
9266  mu += 0.0;
9267 
9268  if (FlagQuadraticTerms) {
9269  //Add contributions that are quadratic in the effective coefficients
9270  mu += 0.0;
9271 
9272  }
9273 
9274  } else if (sqrt_s == 27.0) {
9275 
9276  C1 = 0.0;
9277 
9278  mu += 0.0;
9279 
9280  if (FlagQuadraticTerms) {
9281  //Add contributions that are quadratic in the effective coefficients
9282  mu += 0.0;
9283 
9284  }
9285 
9286  } else if (sqrt_s == 100.0) {
9287 
9288  C1 = 0.0;
9289 
9290  mu += 0.0;
9291 
9292  if (FlagQuadraticTerms) {
9293  //Add contributions that are quadratic in the effective coefficients
9294  mu += 0.0;
9295 
9296  }
9297 
9298  } else
9299  throw std::runtime_error("Bad argument in NPSMEFTd6::mutHq()");
9300 
9301  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
9302  //mu += etHqint + etHqpar;
9303 
9304 // Linear contribution from Higgs self-coupling
9305  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
9306 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
9308 
9309  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9310 
9311  return mu;
9312 }

◆ muTHUggHbb()

double NPSMEFTd6::muTHUggHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,bb}\)

Reimplemented from NPbase.

Definition at line 13692 of file NPSMEFTd6.cpp.

13693 {
13694  if (FlagQuadraticTerms) {
13695  return ( muggH(sqrt_s)*BrHbbRatio() * (1.0 + eggFHbb ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHbbint + eHbbpar) );
13696  } else {
13697  return ( muggH(sqrt_s) + BrHbbRatio() - 1.0 + eggFHbb - eggFint - eggFpar - eHbbint - eHbbpar + eHwidth );
13698  }
13699 }

◆ muTHUggHgaga()

double NPSMEFTd6::muTHUggHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 13188 of file NPSMEFTd6.cpp.

13189 {
13190  if (FlagQuadraticTerms) {
13191  return ( muggH(sqrt_s)*BrHgagaRatio() * (1.0 + eggFHgaga ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHgagaint + eHgagapar) );
13192  } else {
13193  return ( muggH(sqrt_s) + BrHgagaRatio() - 1.0 + eggFHgaga - eggFint - eggFpar - eHgagaint - eHgagapar + eHwidth );
13194  }
13195 }

◆ muTHUggHmumu()

double NPSMEFTd6::muTHUggHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13566 of file NPSMEFTd6.cpp.

13567 {
13568  if (FlagQuadraticTerms) {
13569  return ( muggH(sqrt_s)*BrHmumuRatio() * (1.0 + eggFHmumu ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHmumuint + eHmumupar) );
13570  } else {
13571  return ( muggH(sqrt_s) + BrHmumuRatio() - 1.0 + eggFHmumu - eggFint - eggFpar - eHmumuint - eHmumupar + eHwidth );
13572  }
13573 }

◆ muTHUggHtautau()

double NPSMEFTd6::muTHUggHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13629 of file NPSMEFTd6.cpp.

13630 {
13631  if (FlagQuadraticTerms) {
13632  return ( muggH(sqrt_s)*BrHtautauRatio() * (1.0 + eggFHtautau ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHtautauint + eHtautaupar) );
13633  } else {
13634  return ( muggH(sqrt_s) + BrHtautauRatio() - 1.0 + eggFHtautau - eggFint - eggFpar - eHtautauint - eHtautaupar + eHwidth );
13635  }
13636 }

◆ muTHUggHWW()

double NPSMEFTd6::muTHUggHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW}\)

Reimplemented from NPbase.

Definition at line 13440 of file NPSMEFTd6.cpp.

13441 {
13442  if (FlagQuadraticTerms) {
13443  return ( muggH(sqrt_s)*BrHWWRatio() * (1.0 + eggFHWW ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHWWint + eHWWpar) );
13444  } else {
13445  return ( muggH(sqrt_s) + BrHWWRatio() - 1.0 + eggFHWW - eggFint - eggFpar - eHWWint - eHWWpar + eHwidth );
13446  }
13447 }

◆ muTHUggHWW2l2v()

double NPSMEFTd6::muTHUggHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13503 of file NPSMEFTd6.cpp.

13504 {
13505  if (FlagQuadraticTerms) {
13506  return ( muggH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eggFHWW ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHWWint + eHWWpar) );
13507  } else {
13508  return ( muggH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eggFHWW - eggFint - eggFpar - eHWWint - eHWWpar + eHwidth );
13509  }
13510 }

◆ muTHUggHZga()

double NPSMEFTd6::muTHUggHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 13251 of file NPSMEFTd6.cpp.

13252 {
13253  if (FlagQuadraticTerms) {
13254  return ( muggH(sqrt_s)*BrHZgaRatio() * (1.0 + eggFHZga ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZgaint + eHZgapar) );
13255  } else {
13256  return ( muggH(sqrt_s) + BrHZgaRatio() - 1.0 + eggFHZga - eggFint - eggFpar - eHZgaint - eHZgapar + eHwidth );
13257  }
13258 }

◆ muTHUggHZgamumu()

double NPSMEFTd6::muTHUggHZgamumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,Z\gamma\to \gamma 2\mu}\)

Reimplemented from NPbase.

Definition at line 13807 of file NPSMEFTd6.cpp.

13808 {
13809  if (FlagQuadraticTerms) {
13810  return ( muggH(sqrt_s)*BrHZgamumuRatio() * (1.0 + eggFHZga ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZgaint + eHZgapar) );
13811  } else {
13812  return ( muggH(sqrt_s) + BrHZgamumuRatio() - 1.0 + eggFHZga - eggFint - eggFpar - eHZgaint - eHZgapar + eHwidth );
13813  }
13814 }

◆ muTHUggHZZ()

double NPSMEFTd6::muTHUggHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13314 of file NPSMEFTd6.cpp.

13315 {
13316  if (FlagQuadraticTerms) {
13317  return ( muggH(sqrt_s)*BrHZZRatio() * (1.0 + eggFHZZ ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZZint + eHZZpar) );
13318  } else {
13319  return ( muggH(sqrt_s) + BrHZZRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth );
13320  }
13321 }

◆ muTHUggHZZ4l()

double NPSMEFTd6::muTHUggHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13377 of file NPSMEFTd6.cpp.

13378 {
13379  if (FlagQuadraticTerms) {
13380  return ( muggH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eggFHZZ ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZZint + eHZZpar) );
13381  } else {
13382  return ( muggH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth );
13383  }
13384 }

◆ muTHUggHZZ4mu()

double NPSMEFTd6::muTHUggHZZ4mu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ggH,ZZ\to 4\mu}\)

Reimplemented from NPbase.

Definition at line 13798 of file NPSMEFTd6.cpp.

13799 {
13800  if (FlagQuadraticTerms) {
13801  return ( muggH(sqrt_s)*BrHZZ4muRatio() * (1.0 + eggFHZZ ) * (1.0 + eHwidth)/(1.0 + eggFint + eggFpar)/(1.0 + eHZZint + eHZZpar) );
13802  } else {
13803  return ( muggH(sqrt_s) + BrHZZ4muRatio() - 1.0 + eggFHZZ - eggFint - eggFpar - eHZZint - eHZZpar + eHwidth );
13804  }
13805 }

◆ muTHUttHbb()

double NPSMEFTd6::muTHUttHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,bb}\)

Reimplemented from NPbase.

Definition at line 13746 of file NPSMEFTd6.cpp.

13747 {
13748  if (FlagQuadraticTerms) {
13749  return ( muttH(sqrt_s)*BrHbbRatio() * (1.0 + ettHbb ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHbbint + eHbbpar) );
13750  } else {
13751  return ( muttH(sqrt_s) + BrHbbRatio() - 1.0 + ettHbb - eeettHint - eeettHpar - eHbbint - eHbbpar + eHwidth );
13752  }
13753 }

◆ muTHUttHgaga()

double NPSMEFTd6::muTHUttHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 13242 of file NPSMEFTd6.cpp.

13243 {
13244  if (FlagQuadraticTerms) {
13245  return ( muttH(sqrt_s)*BrHgagaRatio() * (1.0 + ettHgaga ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHgagaint + eHgagapar) );
13246  } else {
13247  return ( muttH(sqrt_s) + BrHgagaRatio() - 1.0 + ettHgaga - eeettHint - eeettHpar - eHgagaint - eHgagapar + eHwidth );
13248  }
13249 }

◆ muTHUttHmumu()

double NPSMEFTd6::muTHUttHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13620 of file NPSMEFTd6.cpp.

13621 {
13622  if (FlagQuadraticTerms) {
13623  return ( muttH(sqrt_s)*BrHmumuRatio() * (1.0 + ettHmumu ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHmumuint + eHmumupar) );
13624  } else {
13625  return ( muttH(sqrt_s) + BrHmumuRatio() - 1.0 + ettHmumu - eeettHint - eeettHpar - eHmumuint - eHmumupar + eHwidth );
13626  }
13627 }

◆ muTHUttHtautau()

double NPSMEFTd6::muTHUttHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13683 of file NPSMEFTd6.cpp.

13684 {
13685  if (FlagQuadraticTerms) {
13686  return ( muttH(sqrt_s)*BrHtautauRatio() * (1.0 + ettHtautau ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHtautauint + eHtautaupar) );
13687  } else {
13688  return ( muttH(sqrt_s) + BrHtautauRatio() - 1.0 + ettHtautau - eeettHint - eeettHpar - eHtautauint - eHtautaupar + eHwidth );
13689  }
13690 }

◆ muTHUttHWW()

double NPSMEFTd6::muTHUttHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW}\)

Reimplemented from NPbase.

Definition at line 13494 of file NPSMEFTd6.cpp.

13495 {
13496  if (FlagQuadraticTerms) {
13497  return ( muttH(sqrt_s)*BrHWWRatio() * (1.0 + ettHWW ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHWWint + eHWWpar) );
13498  } else {
13499  return ( muttH(sqrt_s) + BrHWWRatio() - 1.0 + ettHWW - eeettHint - eeettHpar - eHWWint - eHWWpar + eHwidth );
13500  }
13501 }

◆ muTHUttHWW2l2v()

double NPSMEFTd6::muTHUttHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13557 of file NPSMEFTd6.cpp.

13558 {
13559  if (FlagQuadraticTerms) {
13560  return ( muttH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + ettHWW ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHWWint + eHWWpar) );
13561  } else {
13562  return ( muttH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + ettHWW - eeettHint - eeettHpar - eHWWint - eHWWpar + eHwidth );
13563  }
13564 }

◆ muTHUttHZga()

double NPSMEFTd6::muTHUttHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 13305 of file NPSMEFTd6.cpp.

13306 {
13307  if (FlagQuadraticTerms) {
13308  return ( muttH(sqrt_s)*BrHZgaRatio() * (1.0 + ettHZga ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHZgaint + eHZgapar) );
13309  } else {
13310  return ( muttH(sqrt_s) + BrHZgaRatio() - 1.0 + ettHZga - eeettHint - eeettHpar - eHZgaint - eHZgapar + eHwidth );
13311  }
13312 }

◆ muTHUttHZZ()

double NPSMEFTd6::muTHUttHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13368 of file NPSMEFTd6.cpp.

13369 {
13370  if (FlagQuadraticTerms) {
13371  return ( muttH(sqrt_s)*BrHZZRatio() * (1.0 + ettHZZ ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHZZint + eHZZpar) );
13372  } else {
13373  return ( muttH(sqrt_s) + BrHZZRatio() - 1.0 + ettHZZ - eeettHint - eeettHpar - eHZZint - eHZZpar + eHwidth );
13374  }
13375 }

◆ muTHUttHZZ4l()

double NPSMEFTd6::muTHUttHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13431 of file NPSMEFTd6.cpp.

13432 {
13433  if (FlagQuadraticTerms) {
13434  return ( muttH(sqrt_s)*BrHZZ4lRatio() * (1.0 + ettHZZ ) * (1.0 + eHwidth)/(1.0 + eeettHint + eeettHpar)/(1.0 + eHZZint + eHZZpar) );
13435  } else {
13436  return ( muttH(sqrt_s) + BrHZZ4lRatio() - 1.0 + ettHZZ - eeettHint - eeettHpar - eHZZint - eHZZpar + eHwidth );
13437  }
13438 }

◆ muTHUVBFBRinv()

double NPSMEFTd6::muTHUVBFBRinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF}BR_{inv}\)

Reimplemented from NPbase.

Definition at line 13755 of file NPSMEFTd6.cpp.

13756 {
13757  return ( muVBF(sqrt_s)*Br_H_inv() * (1.0 + eVBFHinv )/(1.0 + eVBFint + eVBFpar) );
13758 }

◆ muTHUVBFHbb()

double NPSMEFTd6::muTHUVBFHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,bb}\)

Reimplemented from NPbase.

Definition at line 13701 of file NPSMEFTd6.cpp.

13702 {
13703  if (FlagQuadraticTerms) {
13704  return ( muVBF(sqrt_s)*BrHbbRatio() * (1.0 + eVBFHbb ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHbbint + eHbbpar) );
13705  } else {
13706  return ( muVBF(sqrt_s) + BrHbbRatio() - 1.0 + eVBFHbb - eVBFint - eVBFpar - eHbbint - eHbbpar + eHwidth );
13707  }
13708 }

◆ muTHUVBFHgaga()

double NPSMEFTd6::muTHUVBFHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 13197 of file NPSMEFTd6.cpp.

13198 {
13199  if (FlagQuadraticTerms) {
13200  return ( muVBF(sqrt_s)*BrHgagaRatio() * (1.0 + eVBFHgaga ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHgagaint + eHgagapar) );
13201  } else {
13202  return ( muVBF(sqrt_s) + BrHgagaRatio() - 1.0 + eVBFHgaga - eVBFint - eVBFpar - eHgagaint - eHgagapar + eHwidth );
13203  }
13204 }

◆ muTHUVBFHinv()

double NPSMEFTd6::muTHUVBFHinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,inv}\)

Reimplemented from NPbase.

Definition at line 13760 of file NPSMEFTd6.cpp.

13761 {
13762  if (FlagQuadraticTerms) {
13763  return ( muVBF(sqrt_s)*BrHtoinvRatio() * (1.0 + eVBFHinv )/(1.0 + eVBFint + eVBFpar) );
13764  } else {
13765  return ( muVBF(sqrt_s) + BrHtoinvRatio() - 1.0 + eVBFHinv - eVBFint - eVBFpar );
13766  }
13767 }

◆ muTHUVBFHmumu()

double NPSMEFTd6::muTHUVBFHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13575 of file NPSMEFTd6.cpp.

13576 {
13577  if (FlagQuadraticTerms) {
13578  return ( muVBF(sqrt_s)*BrHmumuRatio() * (1.0 + eVBFHmumu ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHmumuint + eHmumupar) );
13579  } else {
13580  return ( muVBF(sqrt_s) + BrHmumuRatio() - 1.0 + eVBFHmumu - eVBFint - eVBFpar - eHmumuint - eHmumupar + eHwidth );
13581  }
13582 }

◆ muTHUVBFHtautau()

double NPSMEFTd6::muTHUVBFHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13638 of file NPSMEFTd6.cpp.

13639 {
13640  if (FlagQuadraticTerms) {
13641  return ( muVBF(sqrt_s)*BrHtautauRatio() * (1.0 + eVBFHtautau ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHtautauint + eHtautaupar) );
13642  } else {
13643  return ( muVBF(sqrt_s) + BrHtautauRatio() - 1.0 + eVBFHtautau - eVBFint - eVBFpar - eHtautauint - eHtautaupar + eHwidth );
13644  }
13645 }

◆ muTHUVBFHWW()

double NPSMEFTd6::muTHUVBFHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW}\)

Reimplemented from NPbase.

Definition at line 13449 of file NPSMEFTd6.cpp.

13450 {
13451  if (FlagQuadraticTerms) {
13452  return ( muVBF(sqrt_s)*BrHWWRatio() * (1.0 + eVBFHWW ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHWWint + eHWWpar) );
13453  } else {
13454  return ( muVBF(sqrt_s) + BrHWWRatio() - 1.0 + eVBFHWW - eVBFint - eVBFpar - eHWWint - eHWWpar + eHwidth );
13455  }
13456 }

◆ muTHUVBFHWW2l2v()

double NPSMEFTd6::muTHUVBFHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13512 of file NPSMEFTd6.cpp.

13513 {
13514  if (FlagQuadraticTerms) {
13515  return ( muVBF(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eVBFHWW ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHWWint + eHWWpar) );
13516  } else {
13517  return ( muVBF(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eVBFHWW - eVBFint - eVBFpar - eHWWint - eHWWpar + eHwidth );
13518  }
13519 }

◆ muTHUVBFHZga()

double NPSMEFTd6::muTHUVBFHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 13260 of file NPSMEFTd6.cpp.

13261 {
13262  if (FlagQuadraticTerms) {
13263  return ( muVBF(sqrt_s)*BrHZgaRatio() * (1.0 + eVBFHZga ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHZgaint + eHZgapar) );
13264  } else {
13265  return ( muVBF(sqrt_s) + BrHZgaRatio() - 1.0 + eVBFHZga - eVBFint - eVBFpar - eHZgaint - eHZgapar + eHwidth );
13266  }
13267 }

◆ muTHUVBFHZZ()

double NPSMEFTd6::muTHUVBFHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ}\)

Reimplemented from NPbase.

Definition at line 13323 of file NPSMEFTd6.cpp.

13324 {
13325  if (FlagQuadraticTerms) {
13326  return ( muVBF(sqrt_s)*BrHZZRatio() * (1.0 + eVBFHZZ ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHZZint + eHZZpar) );
13327  } else {
13328  return ( muVBF(sqrt_s) + BrHZZRatio() - 1.0 + eVBFHZZ - eVBFint - eVBFpar - eHZZint - eHZZpar + eHwidth );
13329  }
13330 }

◆ muTHUVBFHZZ4l()

double NPSMEFTd6::muTHUVBFHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13386 of file NPSMEFTd6.cpp.

13387 {
13388  if (FlagQuadraticTerms) {
13389  return ( muVBF(sqrt_s)*BrHZZ4lRatio() * (1.0 + eVBFHZZ ) * (1.0 + eHwidth)/(1.0 + eVBFint + eVBFpar)/(1.0 + eHZZint + eHZZpar) );
13390  } else {
13391  return ( muVBF(sqrt_s) + BrHZZ4lRatio() - 1.0 + eVBFHZZ - eVBFint - eVBFpar - eHZZint - eHZZpar + eHwidth );
13392  }
13393 }

◆ muTHUVHbb()

double NPSMEFTd6::muTHUVHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,bb}\)

Reimplemented from NPbase.

Definition at line 13728 of file NPSMEFTd6.cpp.

13729 {
13730  // Theory uncertainty in VH production, from the WH and ZH ones
13731  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13732  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13733  double eVHtot,eVHbb;
13734 
13735  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13736 
13737  eVHbb = (eWHbb * sigmaWH_SM + eZHbb * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13738 
13739  if (FlagQuadraticTerms) {
13740  return ( muVH(sqrt_s)*BrHbbRatio() * (1.0 + eVHbb ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHbbint + eHbbpar) );
13741  } else {
13742  return ( muVH(sqrt_s) + BrHbbRatio() - 1.0 + eVHbb - eVHtot - eHbbint - eHbbpar + eHwidth );
13743  }
13744 }

◆ muTHUVHBRinv()

double NPSMEFTd6::muTHUVHBRinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH}BR_{inv}\)

Reimplemented from NPbase.

Definition at line 13769 of file NPSMEFTd6.cpp.

13770 {
13771  // Theory uncertainty in VH production, from the WH and ZH ones
13772  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13773  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13774  double eVHtot;
13775 
13776  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13777 
13778  return ( muVH(sqrt_s)*Br_H_inv() * (1.0 + eVHinv )/(1.0 + eVHtot) );
13779 }

◆ muTHUVHgaga()

double NPSMEFTd6::muTHUVHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 13224 of file NPSMEFTd6.cpp.

13225 {
13226  // Theory uncertainty in VH production, from the WH and ZH ones
13227  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13228  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13229  double eVHtot,eVHgaga;
13230 
13231  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13232 
13233  eVHgaga = (eWHgaga * sigmaWH_SM + eZHgaga * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13234 
13235  if (FlagQuadraticTerms) {
13236  return ( muVH(sqrt_s)*BrHgagaRatio() * (1.0 + eVHgaga ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHgagaint + eHgagapar) );
13237  } else {
13238  return ( muVH(sqrt_s) + BrHgagaRatio() - 1.0 + eVHgaga - eVHtot - eHgagaint - eHgagapar + eHwidth );
13239  }
13240 }

◆ muTHUVHinv()

double NPSMEFTd6::muTHUVHinv ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,inv}\)

Reimplemented from NPbase.

Definition at line 13781 of file NPSMEFTd6.cpp.

13782 {
13783  // Theory uncertainty in VH production, from the WH and ZH ones
13784  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13785  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13786  double eVHtot;
13787 
13788  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13789 
13790  if (FlagQuadraticTerms) {
13791  return ( muVH(sqrt_s)*BrHtoinvRatio() * (1.0 + eVHinv )/(1.0 + eVHtot) );
13792  } else {
13793  return ( muVH(sqrt_s) + BrHtoinvRatio() - 1.0 + eVHinv - eVHtot );
13794  }
13795 }

◆ muTHUVHmumu()

double NPSMEFTd6::muTHUVHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13602 of file NPSMEFTd6.cpp.

13603 {
13604  // Theory uncertainty in VH production, from the WH and ZH ones
13605  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13606  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13607  double eVHtot,eVHmumu;
13608 
13609  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13610 
13611  eVHmumu = (eWHmumu * sigmaWH_SM + eZHmumu * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13612 
13613  if (FlagQuadraticTerms) {
13614  return ( muVH(sqrt_s)*BrHmumuRatio() * (1.0 + eVHmumu ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHmumuint + eHmumupar) );
13615  } else {
13616  return ( muVH(sqrt_s) + BrHmumuRatio() - 1.0 + eVHmumu - eVHtot - eHmumuint - eHmumupar + eHwidth );
13617  }
13618 }

◆ muTHUVHtautau()

double NPSMEFTd6::muTHUVHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13665 of file NPSMEFTd6.cpp.

13666 {
13667  // Theory uncertainty in VH production, from the WH and ZH ones
13668  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13669  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13670  double eVHtot,eVHtautau;
13671 
13672  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13673 
13674  eVHtautau = (eWHtautau * sigmaWH_SM + eZHtautau * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13675 
13676  if (FlagQuadraticTerms) {
13677  return ( muVH(sqrt_s)*BrHtautauRatio() * (1.0 + eVHtautau ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHtautauint + eHtautaupar) );
13678  } else {
13679  return ( muVH(sqrt_s) + BrHtautauRatio() - 1.0 + eVHtautau - eVHtot - eHtautauint - eHtautaupar + eHwidth );
13680  }
13681 }

◆ muTHUVHWW()

double NPSMEFTd6::muTHUVHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW}\)

Reimplemented from NPbase.

Definition at line 13476 of file NPSMEFTd6.cpp.

13477 {
13478  // Theory uncertainty in VH production, from the WH and ZH ones
13479  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13480  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13481  double eVHtot,eVHWW;
13482 
13483  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13484 
13485  eVHWW = (eWHWW * sigmaWH_SM + eZHWW * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13486 
13487  if (FlagQuadraticTerms) {
13488  return ( muVH(sqrt_s)*BrHWWRatio() * (1.0 + eVHWW ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHWWint + eHWWpar) );
13489  } else {
13490  return ( muVH(sqrt_s) + BrHWWRatio() - 1.0 + eVHWW - eVHtot - eHWWint - eHWWpar + eHwidth );
13491  }
13492 }

◆ muTHUVHWW2l2v()

double NPSMEFTd6::muTHUVHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13539 of file NPSMEFTd6.cpp.

13540 {
13541  // Theory uncertainty in VH production, from the WH and ZH ones
13542  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13543  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13544  double eVHtot,eVHWW;
13545 
13546  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13547 
13548  eVHWW = (eWHWW * sigmaWH_SM + eZHWW * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13549 
13550  if (FlagQuadraticTerms) {
13551  return ( muVH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eVHWW ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHWWint + eHWWpar) );
13552  } else {
13553  return ( muVH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eVHWW - eVHtot - eHWWint - eHWWpar + eHwidth );
13554  }
13555 }

◆ muTHUVHZga()

double NPSMEFTd6::muTHUVHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 13287 of file NPSMEFTd6.cpp.

13288 {
13289  // Theory uncertainty in VH production, from the WH and ZH ones
13290  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13291  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13292  double eVHtot,eVHZga;
13293 
13294  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13295 
13296  eVHZga = (eWHZga * sigmaWH_SM + eZHZga * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13297 
13298  if (FlagQuadraticTerms) {
13299  return ( muVH(sqrt_s)*BrHZgaRatio() * (1.0 + eVHZga ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHZgaint + eHZgapar) );
13300  } else {
13301  return ( muVH(sqrt_s) + BrHZgaRatio() - 1.0 + eVHZga - eVHtot - eHZgaint - eHZgapar + eHwidth );
13302  }
13303 }

◆ muTHUVHZZ()

double NPSMEFTd6::muTHUVHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13350 of file NPSMEFTd6.cpp.

13351 {
13352  // Theory uncertainty in VH production, from the WH and ZH ones
13353  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13354  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13355  double eVHtot,eVHZZ;
13356 
13357  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13358 
13359  eVHZZ = (eWHZZ * sigmaWH_SM + eZHZZ * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13360 
13361  if (FlagQuadraticTerms) {
13362  return ( muVH(sqrt_s)*BrHZZRatio() * (1.0 + eVHZZ ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHZZint + eHZZpar) );
13363  } else {
13364  return ( muVH(sqrt_s) + BrHZZRatio() - 1.0 + eVHZZ - eVHtot - eHZZint - eHZZpar + eHwidth );
13365  }
13366 }

◆ muTHUVHZZ4l()

double NPSMEFTd6::muTHUVHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13413 of file NPSMEFTd6.cpp.

13414 {
13415  // Theory uncertainty in VH production, from the WH and ZH ones
13416  double sigmaWH_SM = trueSM.computeSigmaWH(sqrt_s);
13417  double sigmaZH_SM = trueSM.computeSigmaZH(sqrt_s);
13418  double eVHtot,eVHZZ;
13419 
13420  eVHtot = ((eWHint + eWHpar) * sigmaWH_SM + (eZHint + eZHpar) * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13421 
13422  eVHZZ = (eWHZZ * sigmaWH_SM + eZHZZ * sigmaZH_SM) / (sigmaWH_SM + sigmaZH_SM);
13423 
13424  if (FlagQuadraticTerms) {
13425  return ( muVH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eVHZZ ) * (1.0 + eHwidth)/(1.0 + eVHtot)/(1.0 + eHZZint + eHZZpar) );
13426  } else {
13427  return ( muVH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eVHZZ - eVHtot - eHZZint - eHZZpar + eHwidth );
13428  }
13429 }

◆ muTHUWHbb()

double NPSMEFTd6::muTHUWHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,bb}\)

Reimplemented from NPbase.

Definition at line 13719 of file NPSMEFTd6.cpp.

13720 {
13721  if (FlagQuadraticTerms) {
13722  return ( muWH(sqrt_s)*BrHbbRatio() * (1.0 + eWHbb ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHbbint + eHbbpar) );
13723  } else {
13724  return ( muWH(sqrt_s) + BrHbbRatio() - 1.0 + eWHbb - eWHint - eWHpar - eHbbint - eHbbpar + eHwidth );
13725  }
13726 }

◆ muTHUWHgaga()

double NPSMEFTd6::muTHUWHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 13215 of file NPSMEFTd6.cpp.

13216 {
13217  if (FlagQuadraticTerms) {
13218  return ( muWH(sqrt_s)*BrHgagaRatio() * (1.0 + eWHgaga ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHgagaint + eHgagapar) );
13219  } else {
13220  return ( muWH(sqrt_s) + BrHgagaRatio() - 1.0 + eWHgaga - eWHint - eWHpar - eHgagaint - eHgagapar + eHwidth );
13221  }
13222 }

◆ muTHUWHmumu()

double NPSMEFTd6::muTHUWHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13593 of file NPSMEFTd6.cpp.

13594 {
13595  if (FlagQuadraticTerms) {
13596  return ( muWH(sqrt_s)*BrHmumuRatio() * (1.0 + eWHmumu ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHmumuint + eHmumupar) );
13597  } else {
13598  return ( muWH(sqrt_s) + BrHmumuRatio() - 1.0 + eWHmumu - eWHint - eWHpar - eHmumuint - eHmumupar + eHwidth );
13599  }
13600 }

◆ muTHUWHtautau()

double NPSMEFTd6::muTHUWHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13656 of file NPSMEFTd6.cpp.

13657 {
13658  if (FlagQuadraticTerms) {
13659  return ( muWH(sqrt_s)*BrHtautauRatio() * (1.0 + eWHtautau ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHtautauint + eHtautaupar) );
13660  } else {
13661  return ( muWH(sqrt_s) + BrHtautauRatio() - 1.0 + eWHtautau - eWHint - eWHpar - eHtautauint - eHtautaupar + eHwidth );
13662  }
13663 }

◆ muTHUWHWW()

double NPSMEFTd6::muTHUWHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW}\)

Reimplemented from NPbase.

Definition at line 13467 of file NPSMEFTd6.cpp.

13468 {
13469  if (FlagQuadraticTerms) {
13470  return ( muWH(sqrt_s)*BrHWWRatio() * (1.0 + eWHWW ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHWWint + eHWWpar) );
13471  } else {
13472  return ( muWH(sqrt_s) + BrHWWRatio() - 1.0 + eWHWW - eWHint - eWHpar - eHWWint - eHWWpar + eHwidth );
13473  }
13474 }

◆ muTHUWHWW2l2v()

double NPSMEFTd6::muTHUWHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13530 of file NPSMEFTd6.cpp.

13531 {
13532  if (FlagQuadraticTerms) {
13533  return ( muWH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eWHWW ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHWWint + eHWWpar) );
13534  } else {
13535  return ( muWH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eWHWW - eWHint - eWHpar - eHWWint - eHWWpar + eHwidth );
13536  }
13537 }

◆ muTHUWHZga()

double NPSMEFTd6::muTHUWHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 13278 of file NPSMEFTd6.cpp.

13279 {
13280  if (FlagQuadraticTerms) {
13281  return ( muWH(sqrt_s)*BrHZgaRatio() * (1.0 + eWHZga ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHZgaint + eHZgapar) );
13282  } else {
13283  return ( muWH(sqrt_s) + BrHZgaRatio() - 1.0 + eWHZga - eWHint - eWHpar - eHZgaint - eHZgapar + eHwidth );
13284  }
13285 }

◆ muTHUWHZZ()

double NPSMEFTd6::muTHUWHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13341 of file NPSMEFTd6.cpp.

13342 {
13343  if (FlagQuadraticTerms) {
13344  return ( muWH(sqrt_s)*BrHZZRatio() * (1.0 + eWHZZ ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHZZint + eHZZpar) );
13345  } else {
13346  return ( muWH(sqrt_s) + BrHZZRatio() - 1.0 + eWHZZ - eWHint - eWHpar - eHZZint - eHZZpar + eHwidth );
13347  }
13348 }

◆ muTHUWHZZ4l()

double NPSMEFTd6::muTHUWHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13404 of file NPSMEFTd6.cpp.

13405 {
13406  if (FlagQuadraticTerms) {
13407  return ( muWH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eWHZZ ) * (1.0 + eHwidth)/(1.0 + eWHint + eWHpar)/(1.0 + eHZZint + eHZZpar) );
13408  } else {
13409  return ( muWH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eWHZZ - eWHint - eWHpar - eHZZint - eHZZpar + eHwidth );
13410  }
13411 }

◆ muTHUZHbb()

double NPSMEFTd6::muTHUZHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,bb}\)

Reimplemented from NPbase.

Definition at line 13710 of file NPSMEFTd6.cpp.

13711 {
13712  if (FlagQuadraticTerms) {
13713  return ( muZH(sqrt_s)*BrHbbRatio() * (1.0 + eZHbb ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHbbint + eHbbpar) );
13714  } else {
13715  return ( muZH(sqrt_s) + BrHbbRatio() - 1.0 + eZHbb - eZHint - eZHpar - eHbbint - eHbbpar + eHwidth );
13716  }
13717 }

◆ muTHUZHgaga()

double NPSMEFTd6::muTHUZHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 13206 of file NPSMEFTd6.cpp.

13207 {
13208  if (FlagQuadraticTerms) {
13209  return ( muZH(sqrt_s)*BrHgagaRatio() * (1.0 + eZHgaga ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHgagaint + eHgagapar) );
13210  } else {
13211  return ( muZH(sqrt_s) + BrHgagaRatio() - 1.0 + eZHgaga - eZHint - eZHpar - eHgagaint - eHgagapar + eHwidth );
13212  }
13213 }

◆ muTHUZHmumu()

double NPSMEFTd6::muTHUZHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13584 of file NPSMEFTd6.cpp.

13585 {
13586  if (FlagQuadraticTerms) {
13587  return ( muZH(sqrt_s)*BrHmumuRatio() * (1.0 + eZHmumu ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHmumuint + eHmumupar) );
13588  } else {
13589  return ( muZH(sqrt_s) + BrHmumuRatio() - 1.0 + eZHmumu - eZHint - eZHpar - eHmumuint - eHmumupar + eHwidth );
13590  }
13591 }

◆ muTHUZHtautau()

double NPSMEFTd6::muTHUZHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13647 of file NPSMEFTd6.cpp.

13648 {
13649  if (FlagQuadraticTerms) {
13650  return ( muZH(sqrt_s)*BrHtautauRatio() * (1.0 + eZHtautau ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHtautauint + eHtautaupar) );
13651  } else {
13652  return ( muZH(sqrt_s) + BrHtautauRatio() - 1.0 + eZHtautau - eZHint - eZHpar - eHtautauint - eHtautaupar + eHwidth );
13653  }
13654 }

◆ muTHUZHWW()

double NPSMEFTd6::muTHUZHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW}\)

Reimplemented from NPbase.

Definition at line 13458 of file NPSMEFTd6.cpp.

13459 {
13460  if (FlagQuadraticTerms) {
13461  return ( muZH(sqrt_s)*BrHWWRatio() * (1.0 + eZHWW ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHWWint + eHWWpar) );
13462  } else {
13463  return ( muZH(sqrt_s) + BrHWWRatio() - 1.0 + eZHWW - eZHint - eZHpar - eHWWint - eHWWpar + eHwidth );
13464  }
13465 }

◆ muTHUZHWW2l2v()

double NPSMEFTd6::muTHUZHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13521 of file NPSMEFTd6.cpp.

13522 {
13523  if (FlagQuadraticTerms) {
13524  return ( muZH(sqrt_s)*BrHWW2l2vRatio() * (1.0 + eZHWW ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHWWint + eHWWpar) );
13525  } else {
13526  return ( muZH(sqrt_s) + BrHWW2l2vRatio() - 1.0 + eZHWW - eZHint - eZHpar - eHWWint - eHWWpar + eHwidth );
13527  }
13528 }

◆ muTHUZHZga()

double NPSMEFTd6::muTHUZHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 13269 of file NPSMEFTd6.cpp.

13270 {
13271  if (FlagQuadraticTerms) {
13272  return ( muZH(sqrt_s)*BrHZgaRatio() * (1.0 + eZHZga ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHZgaint + eHZgapar) );
13273  } else {
13274  return ( muZH(sqrt_s) + BrHZgaRatio() - 1.0 + eZHZga - eZHint - eZHpar - eHZgaint - eHZgapar + eHwidth );
13275  }
13276 }

◆ muTHUZHZZ()

double NPSMEFTd6::muTHUZHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ}\)

Reimplemented from NPbase.

Definition at line 13332 of file NPSMEFTd6.cpp.

13333 {
13334  if (FlagQuadraticTerms) {
13335  return ( muZH(sqrt_s)*BrHZZRatio() * (1.0 + eZHZZ ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHZZint + eHZZpar) );
13336  } else {
13337  return ( muZH(sqrt_s) + BrHZZRatio() - 1.0 + eZHZZ - eZHint - eZHpar - eHZZint - eHZZpar + eHwidth );
13338  }
13339 }

◆ muTHUZHZZ4l()

double NPSMEFTd6::muTHUZHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 13395 of file NPSMEFTd6.cpp.

13396 {
13397  if (FlagQuadraticTerms) {
13398  return ( muZH(sqrt_s)*BrHZZ4lRatio() * (1.0 + eZHZZ ) * (1.0 + eHwidth)/(1.0 + eZHint + eZHpar)/(1.0 + eHZZint + eHZZpar) );
13399  } else {
13400  return ( muZH(sqrt_s) + BrHZZ4lRatio() - 1.0 + eZHZZ - eZHint - eZHpar - eHZZint - eHZZpar + eHwidth );
13401  }
13402 }

◆ muttH()

double NPSMEFTd6::muttH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH}\)

Reimplemented from NPbase.

Definition at line 9078 of file NPSMEFTd6.cpp.

9079 {
9080  double mu = 1.0;
9081 
9082  double C1 = 0.0;
9083 
9084  if (sqrt_s == 1.96) {
9085 
9086  C1 = 0.0; // N.A.
9087 
9088  mu +=
9089  +423420. * (1. + ettH_2_HG ) * CHG / LambdaNP2
9090  -4269.4 * (1. + ettH_2_G ) * CG / LambdaNP2
9091  +566792. * (1. + ettH_2_uG_33r ) * CiuG_33r / LambdaNP2
9092  -2.854 * (1. + ettH_2_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
9093  ;
9094 
9095  if (FlagQuadraticTerms) {
9096  //Add contributions that are quadratic in the effective coefficients
9097  mu += 0.0;
9098 
9099  }
9100 
9101  } else if (sqrt_s == 7.0) {
9102 
9103  C1 = 0.0387;
9104 
9105  mu +=
9106  +532200. * (1. + ettH_78_HG ) * CHG / LambdaNP2
9107  -85145.2 * (1. + ettH_78_G ) * CG / LambdaNP2
9108  +811678. * (1. + ettH_78_uG_33r ) * CiuG_33r / LambdaNP2
9109  -2.841 * (1. + ettH_78_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
9110  ;
9111 
9112  if (FlagQuadraticTerms) {
9113  //Add contributions that are quadratic in the effective coefficients
9114  mu += 0.0;
9115 
9116  }
9117 
9118  } else if (sqrt_s == 8.0) {
9119 
9120  C1 = 0.0378;
9121 
9122  mu +=
9123  +535632. * (1. + ettH_78_HG ) * CHG / LambdaNP2
9124  -86537.2 * (1. + ettH_78_G ) * CG / LambdaNP2
9125  +825379. * (1. + ettH_78_uG_33r ) * CiuG_33r / LambdaNP2
9126  -2.849 * (1. + ettH_78_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
9127  ;
9128 
9129  if (FlagQuadraticTerms) {
9130  //Add contributions that are quadratic in the effective coefficients
9131  mu += 0.0;
9132 
9133  }
9134 
9135  } else if (sqrt_s == 13.0) {
9136 
9137  C1 = 0.0351;
9138 
9139  mu +=
9140  +538764. * (1. + ettH_1314_HG ) * CHG / LambdaNP2
9141  -84648. * (1. + ettH_1314_G ) * CG / LambdaNP2
9142  +860470. * (1. + ettH_1314_uG_33r ) * CiuG_33r / LambdaNP2
9143  -2.834 * (1. + ettH_1314_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
9144  ;
9145 
9146  if (FlagQuadraticTerms) {
9147  //Add contributions that are quadratic in the effective coefficients
9148  mu += 0.0;
9149 
9150  }
9151 
9152  } else if (sqrt_s == 14.0) {
9153 
9154  C1 = 0.0347;
9155 
9156  mu +=
9157  +536600. * (1. + ettH_1314_HG ) * CHG / LambdaNP2
9158  -83824.6 * (1. + ettH_1314_G ) * CG / LambdaNP2
9159  +863670. * (1. + ettH_1314_uG_33r ) * CiuG_33r / LambdaNP2
9160  -2.839 * (1. + ettH_1314_DeltagHt ) * deltaG_hff(quarks[TOP]).real()
9161  ;
9162 
9163  if (FlagQuadraticTerms) {
9164  //Add contributions that are quadratic in the effective coefficients
9165  mu += 0.0;
9166 
9167  }
9168 
9169  } else if (sqrt_s == 27.0) {
9170 
9171  C1 = 0.0320; // From arXiv: 1902.00134
9172 
9173  mu +=
9174  +519682. * CHG / LambdaNP2
9175  -68463.1 * CG / LambdaNP2
9176  +884060. * CiuG_33r / LambdaNP2
9177  -2.849 * deltaG_hff(quarks[TOP]).real()
9178  ;
9179 
9180  if (FlagQuadraticTerms) {
9181  //Add contributions that are quadratic in the effective coefficients
9182  mu += 0.0;
9183 
9184  }
9185 
9186  } else if (sqrt_s == 100.0) {
9187 
9188  C1 = 0.0; // N.A.
9189 
9190  mu +=
9191  +467438. * CHG / LambdaNP2
9192  -22519. * CG / LambdaNP2
9193  +880378. * CiuG_33r / LambdaNP2
9194  -2.837 * deltaG_hff(quarks[TOP]).real()
9195  ;
9196 
9197  if (FlagQuadraticTerms) {
9198  //Add contributions that are quadratic in the effective coefficients
9199  mu += 0.0;
9200 
9201  }
9202 
9203  } else
9204  throw std::runtime_error("Bad argument in NPSMEFTd6::muttH()");
9205 
9206  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
9207  mu += ettHint + ettHpar;
9208 
9209 // Linear contribution from Higgs self-coupling
9210  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
9211 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
9213 
9214  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9215 
9216  return mu;
9217 }

◆ muttHbb()

double NPSMEFTd6::muttHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,bb}\)

Reimplemented from NPbase.

Definition at line 13176 of file NPSMEFTd6.cpp.

13177 {
13178  return muttH(sqrt_s) * BrHbbRatio();
13179 
13180 }

◆ muttHgaga()

double NPSMEFTd6::muttHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12888 of file NPSMEFTd6.cpp.

12889 {
12890  return muttH(sqrt_s) * BrHgagaRatio();
12891 
12892 }

◆ muttHmumu()

double NPSMEFTd6::muttHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13104 of file NPSMEFTd6.cpp.

13105 {
13106  return muttH(sqrt_s) * BrHmumuRatio();
13107 
13108 }

◆ muttHtautau()

double NPSMEFTd6::muttHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13140 of file NPSMEFTd6.cpp.

13141 {
13142  return muttH(sqrt_s) * BrHtautauRatio();
13143 
13144 }

◆ muttHWW()

double NPSMEFTd6::muttHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW}\)

Reimplemented from NPbase.

Definition at line 13032 of file NPSMEFTd6.cpp.

13033 {
13034  return muttH(sqrt_s) * BrHWWRatio();
13035 
13036 }

◆ muttHWW2l2v()

double NPSMEFTd6::muttHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13068 of file NPSMEFTd6.cpp.

13069 {
13070  return muttH(sqrt_s) * BrHWW2l2vRatio();
13071 
13072 }

◆ muttHZbbboost()

double NPSMEFTd6::muttHZbbboost ( const double  sqrt_s) const
virtual

The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\sigma(ttH)/\sigma(ttZ)\) normalized to the SM

Reimplemented from NPbase.

Definition at line 12802 of file NPSMEFTd6.cpp.

12803 {
12804  /* Ratios of BR with the SM*/
12805  double BrHbbrat = BrHbbRatio();
12806  double BrZbbSM = (trueSM.GammaZ(quarks[BOTTOM]))/trueSM.Gamma_Z();
12807  double BrZbbrat = BR_Zf(quarks[BOTTOM])/BrZbbSM;
12808 
12809 // gslpp::complex dKappa_t = deltaG_hff(quarks[TOP]) / (-mtpole / v());
12810 // double dkt = dKappa_t.real();
12811 
12812 // double dgV = deltaGV_f(quarks[TOP]);
12813 // double dgA = deltaGA_f(quarks[TOP]);
12814 // double gLSM = quarks[TOP].getIsospin()
12815 // - (quarks[TOP].getCharge())*sW2_tree;
12816 // double gRSM = - (quarks[TOP].getCharge())*sW2_tree;
12817 
12818 // double dgL = 0.5*(dgV + dgA)/gLSM;
12819 // double dgR = 0.5*(dgV - dgA)/gRSM;
12820 
12821  double dsigmarat;
12822 
12823  /* VERY CRUDE APPROX. */
12824  //dsigmarat = 1.0 +
12825  // 2.0 * dkt -
12826  // 2.0 * (gLSM*gLSM*dgL + gRSM*gRSM*dgR)/(gLSM*gLSM + gRSM*gRSM);
12827 
12828  dsigmarat = 1.0;
12829 // ttH 100 TeV (from muttH func): NOT BOOSTED YET
12830  dsigmarat += +467438. * CHG / LambdaNP2
12831  -22519. * CG / LambdaNP2
12832  +880378. * CiuG_33r / LambdaNP2
12833  -2.837 * deltaG_hff(quarks[TOP]).real()
12834  ;
12835 // Divided (linearized) by ttZ 100 TeV
12836  dsigmarat = dsigmarat - (
12837  -40869.4 * CiHD / LambdaNP2
12838  -52607.9 * CiHWB / LambdaNP2
12839  -90424.9 * CHG / LambdaNP2
12840  +432089. * CG / LambdaNP2
12841  +326525. * CiuG_33r / LambdaNP2
12842  -2028.11 * CiuW_33r / LambdaNP2
12843  +1679.85 * CiuB_33r / LambdaNP2
12844  +1454.5 * CiHQ1_11 / LambdaNP2
12845  +1065.27 * CiHu_11 / LambdaNP2
12846  +82169.1 * CiHu_33 / LambdaNP2
12847  -1229.16 * CiHd_11 / LambdaNP2
12848  +6780.84 * CiHQ3_11 / LambdaNP2
12849  -1.374 * DeltaGF()
12850  +4.242 * -0.5 * (CiHQ1_33 - CiHQ3_33) * v2_over_LambdaNP2
12851  );
12852 
12853  return dsigmarat * (BrHbbrat / BrZbbrat);
12854 
12855 }

◆ muttHZga()

double NPSMEFTd6::muttHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12924 of file NPSMEFTd6.cpp.

12925 {
12926  return muttH(sqrt_s) * BrHZgaRatio();
12927 
12928 }

◆ muttHZZ()

double NPSMEFTd6::muttHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12960 of file NPSMEFTd6.cpp.

12961 {
12962  return muttH(sqrt_s) * BrHZZRatio();
12963 
12964 }

◆ muttHZZ4l()

double NPSMEFTd6::muttHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ttH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12996 of file NPSMEFTd6.cpp.

12997 {
12998  return muttH(sqrt_s) * BrHZZ4lRatio();
12999 
13000 }

◆ muVBF()

double NPSMEFTd6::muVBF ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF}\)

Reimplemented from NPbase.

Definition at line 3758 of file NPSMEFTd6.cpp.

3759 {
3760  double mu = 1.0;
3761 
3762  double C1 = 0.0;
3763 
3764  if (sqrt_s == 1.96) {
3765 
3766  C1 = 0.0; // N.A.
3767 
3768  mu +=
3769  +120936. * (1. + eVBF_2_Hbox ) * CiHbox / LambdaNP2
3770  -9422.68 * (1. + eVBF_2_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3771  -10683.8 * (1. + eVBF_2_Hu_11 ) * CiHu_11 / LambdaNP2
3772  +4055.59 * (1. + eVBF_2_Hd_11 ) * CiHd_11 / LambdaNP2
3773  -229691. * (1. + eVBF_2_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3774  -170093. * (1. + eVBF_2_HD ) * CiHD / LambdaNP2
3775  +8971.22 * (1. + eVBF_2_HB ) * CiHB / LambdaNP2
3776  -65827.6 * (1. + eVBF_2_HW ) * CiHW / LambdaNP2
3777  -323514. * (1. + eVBF_2_HWB ) * CiHWB / LambdaNP2
3778  +481332. * (1. + eVBF_2_HG ) * CHG / LambdaNP2
3779  +1255.16 * (1. + eVBF_2_DHB ) * CiDHB / LambdaNP2
3780  -34956.7 * (1. + eVBF_2_DHW ) * CiDHW / LambdaNP2
3781  -4.511 * (1. + eVBF_2_DeltaGF ) * DeltaGF()
3782  -3.481 * deltaMwd6()
3783  ;
3784 
3785  if (FlagQuadraticTerms) {
3786  //Add contributions that are quadratic in the effective coefficients
3787 
3788  mu += 0.0;
3789 
3790  }
3791 
3792  } else if (sqrt_s == 7.0) {
3793 
3794  C1 = 0.0065;
3795 
3796  mu +=
3797  +121582. * (1. + eVBF_78_Hbox ) * CiHbox / LambdaNP2
3798  +13546.6 * (1. + eVBF_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3799  -27657.6 * (1. + eVBF_78_Hu_11 ) * CiHu_11 / LambdaNP2
3800  +8892.12 * (1. + eVBF_78_Hd_11 ) * CiHd_11 / LambdaNP2
3801  -411400. * (1. + eVBF_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3802  -164286. * (1. + eVBF_78_HD ) * CiHD / LambdaNP2
3803  -423.123 * (1. + eVBF_78_HB ) * CiHB / LambdaNP2
3804  -89854. * (1. + eVBF_78_HW ) * CiHW / LambdaNP2
3805  -312617. * (1. + eVBF_78_HWB ) * CiHWB / LambdaNP2
3806  -82956.8 * (1. + eVBF_78_HG ) * CHG / LambdaNP2
3807  -279.08 * (1. + eVBF_78_DHB ) * CiDHB / LambdaNP2
3808  -54861. * (1. + eVBF_78_DHW ) * CiDHW / LambdaNP2
3809  -4.479 * (1. + eVBF_78_DeltaGF ) * DeltaGF()
3810  -3.22 * deltaMwd6()
3811  ;
3812 
3813  if (FlagQuadraticTerms) {
3814  //Add contributions that are quadratic in the effective coefficients
3815 
3816  mu += 0.0;
3817 
3818  }
3819 
3820  } else if (sqrt_s == 8.0) {
3821 
3822  C1 = 0.0065;
3823 
3824  mu +=
3825  +121042. * (1. + eVBF_78_Hbox ) * CiHbox / LambdaNP2
3826  +12739.3 * (1. + eVBF_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3827  -28367.7 * (1. + eVBF_78_Hu_11 ) * CiHu_11 / LambdaNP2
3828  +9134.21 * (1. + eVBF_78_Hd_11 ) * CiHd_11 / LambdaNP2
3829  -423704. * (1. + eVBF_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3830  -165182. * (1. + eVBF_78_HD ) * CiHD / LambdaNP2
3831  -349.242 * (1. + eVBF_78_HB ) * CiHB / LambdaNP2
3832  -87279.4 * (1. + eVBF_78_HW ) * CiHW / LambdaNP2
3833  -313449. * (1. + eVBF_78_HWB ) * CiHWB / LambdaNP2
3834  -69421.9 * (1. + eVBF_78_HG ) * CHG / LambdaNP2
3835  -373.338 * (1. + eVBF_78_DHB ) * CiDHB / LambdaNP2
3836  -57028.1 * (1. + eVBF_78_DHW ) * CiDHW / LambdaNP2
3837  -4.472 * (1. + eVBF_78_DeltaGF ) * DeltaGF()
3838  -3.138 * deltaMwd6()
3839  ;
3840 
3841  if (FlagQuadraticTerms) {
3842  //Add contributions that are quadratic in the effective coefficients
3843 
3844  mu += 0.0;
3845 
3846  }
3847  } else if (sqrt_s == 13.0) {
3848 
3849  C1 = 0.0064;
3850 
3851  mu +=
3852  +121798. * (1. + eVBF_1314_Hbox ) * CiHbox / LambdaNP2
3853  +10339.7 * (1. + eVBF_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3854  -30827.2 * (1. + eVBF_1314_Hu_11 ) * CiHu_11 / LambdaNP2
3855  +10564.3 * (1. + eVBF_1314_Hd_11 ) * CiHd_11 / LambdaNP2
3856  -466270. * (1. + eVBF_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3857  -164119. * (1. + eVBF_1314_HD ) * CiHD / LambdaNP2
3858  -61.471 * (1. + eVBF_1314_HB ) * CiHB / LambdaNP2
3859  -82985.3 * (1. + eVBF_1314_HW ) * CiHW / LambdaNP2
3860  -313815. * (1. + eVBF_1314_HWB ) * CiHWB / LambdaNP2
3861  -36554. * (1. + eVBF_1314_HG ) * CHG / LambdaNP2
3862  -725.694 * (1. + eVBF_1314_DHB ) * CiDHB / LambdaNP2
3863  -65253.4 * (1. + eVBF_1314_DHW ) * CiDHW / LambdaNP2
3864  -4.474 * (1. + eVBF_1314_DeltaGF ) * DeltaGF()
3865  -3.109 * deltaMwd6()
3866  ;
3867 
3868  if (FlagQuadraticTerms) {
3869  //Add contributions that are quadratic in the effective coefficients
3870  mu += 0.0;
3871  }
3872 
3873  } else if (sqrt_s == 14.0) {
3874 
3875  C1 = 0.0064;
3876 
3877  mu +=
3878  +120948. * (1. + eVBF_1314_Hbox ) * CiHbox / LambdaNP2
3879  +9896.36 * (1. + eVBF_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
3880  -31371. * (1. + eVBF_1314_Hu_11 ) * CiHu_11 / LambdaNP2
3881  +10716.4 * (1. + eVBF_1314_Hd_11 ) * CiHd_11 / LambdaNP2
3882  -473497. * (1. + eVBF_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
3883  -164672. * (1. + eVBF_1314_HD ) * CiHD / LambdaNP2
3884  -60.253 * (1. + eVBF_1314_HB ) * CiHB / LambdaNP2
3885  -83504.9 * (1. + eVBF_1314_HW ) * CiHW / LambdaNP2
3886  -314059. * (1. + eVBF_1314_HWB ) * CiHWB / LambdaNP2
3887  -33627.6 * (1. + eVBF_1314_HG ) * CHG / LambdaNP2
3888  -775.959 * (1. + eVBF_1314_DHB ) * CiDHB / LambdaNP2
3889  -66336.3 * (1. + eVBF_1314_DHW ) * CiDHW / LambdaNP2
3890  -4.474 * (1. + eVBF_1314_DeltaGF ) * DeltaGF()
3891  -3.193 * deltaMwd6()
3892  ;
3893 
3894  if (FlagQuadraticTerms) {
3895  //Add contributions that are quadratic in the effective coefficients
3896  mu += 0.0;
3897 
3898  }
3899 
3900  } else if (sqrt_s == 27.0) {
3901 
3902  C1 = 0.0062; // From arXiv: 1902.00134
3903 
3904  mu +=
3905  +120777. * CiHbox / LambdaNP2
3906  +6664.27 * CiHQ1_11 / LambdaNP2
3907  -34230.7 * CiHu_11 / LambdaNP2
3908  +12917.3 * CiHd_11 / LambdaNP2
3909  -536216. * CiHQ3_11 / LambdaNP2
3910  -163493. * CiHD / LambdaNP2
3911  +58.33 * CiHB / LambdaNP2
3912  -81360.5 * CiHW / LambdaNP2
3913  -313026. * CiHWB / LambdaNP2
3914  -16430. * CHG / LambdaNP2
3915  -1314.45 * CiDHB / LambdaNP2
3916  -75884.6 * CiDHW / LambdaNP2
3917  -4.475 * DeltaGF()
3918  -2.99 * deltaMwd6()
3919  ;
3920 
3921  if (FlagQuadraticTerms) {
3922  //Add contributions that are quadratic in the effective coefficients
3923  mu += 0.0;
3924 
3925  }
3926 
3927  } else if (sqrt_s == 100.0) {
3928 
3929  C1 = 0.0; // N.A.
3930 
3931  mu +=
3932  +121714. * CiHbox / LambdaNP2
3933  -2261.73 * CiHQ1_11 / LambdaNP2
3934  -42045.4 * CiHu_11 / LambdaNP2
3935  +17539.2 * CiHd_11 / LambdaNP2
3936  -674206. * CiHQ3_11 / LambdaNP2
3937  -163344. * CiHD / LambdaNP2
3938  +71.488 * CiHB / LambdaNP2
3939  -90808.2 * CiHW / LambdaNP2
3940  -312544. * CiHWB / LambdaNP2
3941  -8165.65 * CHG / LambdaNP2
3942  -2615.48 * CiDHB / LambdaNP2
3943  -96539.6 * CiDHW / LambdaNP2
3944  -4.452 * DeltaGF()
3945  -2.949 * deltaMwd6()
3946  ;
3947 
3948  if (FlagQuadraticTerms) {
3949  //Add contributions that are quadratic in the effective coefficients
3950  mu += 0.0;
3951 
3952  }
3953 
3954  } else
3955  throw std::runtime_error("Bad argument in NPSMEFTd6::muVBF()");
3956 
3957  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
3958  mu += eVBFint + eVBFpar;
3959 
3960 // Linear contribution from Higgs self-coupling
3961  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
3962 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
3964 
3965  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
3966 
3967  return mu;
3968 }

◆ muVBFgamma()

double NPSMEFTd6::muVBFgamma ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF+\gamma}\)

Reimplemented from NPbase.

Definition at line 3973 of file NPSMEFTd6.cpp.

3974 {
3975  double mu = 1.0;
3976 
3977  double C1 = 0.0; //Use same values as VBF
3978 
3979  if (sqrt_s == 13.0) {
3980 
3981  C1 = 0.0064;
3982 
3983  mu +=
3984  +119630. * CiHbox / LambdaNP2
3985  -501300. * CiHQ3_11 / LambdaNP2
3986  -200890. * CiHD / LambdaNP2
3987  +11852.5 * CiHB / LambdaNP2
3988  -131586. * CiHW / LambdaNP2
3989  -361991. * CiHWB / LambdaNP2
3990  -18894.5 * CiDHB / LambdaNP2
3991  -69025.4 * CiDHW / LambdaNP2
3992  +23773.1 * CiW / LambdaNP2
3993  -4.629 * DeltaGF()
3994  -5.637 * deltaMwd6()
3995  ;
3996 
3997  if (FlagQuadraticTerms) {
3998  //Add contributions that are quadratic in the effective coefficients
3999  mu += 0.0;
4000  }
4001 
4002  } else
4003  throw std::runtime_error("Bad argument in NPSMEFTd6::muVBFgamma()");
4004 
4005  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy. Use same as VBF.)
4006  mu += eVBFint + eVBFpar;
4007 
4008 // Linear contribution from Higgs self-coupling
4009  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
4010 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
4012 
4013  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
4014 
4015  return mu;
4016 }

◆ muVBFHbb()

double NPSMEFTd6::muVBFHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,bb}\)

Reimplemented from NPbase.

Definition at line 13152 of file NPSMEFTd6.cpp.

13153 {
13154  return muVBF(sqrt_s) * BrHbbRatio();
13155 
13156 }

◆ muVBFHgaga()

double NPSMEFTd6::muVBFHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12864 of file NPSMEFTd6.cpp.

12865 {
12866  return muVBF(sqrt_s) * BrHgagaRatio();
12867 
12868 }

◆ muVBFHmumu()

double NPSMEFTd6::muVBFHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13080 of file NPSMEFTd6.cpp.

13081 {
13082  return muVBF(sqrt_s) * BrHmumuRatio();
13083 
13084 }

◆ muVBFHtautau()

double NPSMEFTd6::muVBFHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13116 of file NPSMEFTd6.cpp.

13117 {
13118  return muVBF(sqrt_s) * BrHtautauRatio();
13119 
13120 }

◆ muVBFHWW()

double NPSMEFTd6::muVBFHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW}\)

Reimplemented from NPbase.

Definition at line 13008 of file NPSMEFTd6.cpp.

13009 {
13010  return muVBF(sqrt_s) * BrHWWRatio();
13011 
13012 }

◆ muVBFHWW2l2v()

double NPSMEFTd6::muVBFHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13044 of file NPSMEFTd6.cpp.

13045 {
13046  return muVBF(sqrt_s) * BrHWW2l2vRatio();
13047 
13048 }

◆ muVBFHZga()

double NPSMEFTd6::muVBFHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12900 of file NPSMEFTd6.cpp.

12901 {
12902  return muVBF(sqrt_s) * BrHZgaRatio();
12903 
12904 }

◆ muVBFHZZ()

double NPSMEFTd6::muVBFHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ}\)

Reimplemented from NPbase.

Definition at line 12936 of file NPSMEFTd6.cpp.

12937 {
12938  return muVBF(sqrt_s) * BrHZZRatio();
12939 
12940 }

◆ muVBFHZZ4l()

double NPSMEFTd6::muVBFHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12972 of file NPSMEFTd6.cpp.

12973 {
12974  return muVBF(sqrt_s) * BrHZZ4lRatio();
12975 
12976 }

◆ muVBFpVH()

double NPSMEFTd6::muVBFpVH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VBF+VH}\)

Reimplemented from NPbase.

Definition at line 9063 of file NPSMEFTd6.cpp.

9064 {
9065  double sigmaWH_SM = computeSigmaWH(sqrt_s);
9066  double sigmaZH_SM = computeSigmaZH(sqrt_s);
9067  double sigmaVBF_SM = computeSigmaVBF(sqrt_s);
9068  double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
9069  double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
9070  double sigmaVBF = muVBF(sqrt_s) * sigmaVBF_SM;
9071  double mu = ((sigmaWH + sigmaZH + sigmaVBF) / (sigmaWH_SM + sigmaZH_SM + sigmaVBF_SM));
9072 
9073  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9074 
9075  return mu;
9076 }

◆ muVH()

double NPSMEFTd6::muVH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH}\)

Reimplemented from NPbase.

Definition at line 9050 of file NPSMEFTd6.cpp.

9051 {
9052  double sigmaWH_SM = computeSigmaWH(sqrt_s);
9053  double sigmaZH_SM = computeSigmaZH(sqrt_s);
9054  double sigmaWH = muWH(sqrt_s) * sigmaWH_SM;
9055  double sigmaZH = muZH(sqrt_s) * sigmaZH_SM;
9056  double mu = ((sigmaWH + sigmaZH) / (sigmaWH_SM + sigmaZH_SM));
9057 
9058  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
9059 
9060  return mu;
9061 }

◆ muVHbb()

double NPSMEFTd6::muVHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,bb}\)

Reimplemented from NPbase.

Definition at line 13170 of file NPSMEFTd6.cpp.

13171 {
13172  return muVH(sqrt_s) * BrHbbRatio();
13173 
13174 }

◆ muVHgaga()

double NPSMEFTd6::muVHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12882 of file NPSMEFTd6.cpp.

12883 {
12884  return muVH(sqrt_s) * BrHgagaRatio();
12885 
12886 }

◆ muVHmumu()

double NPSMEFTd6::muVHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13098 of file NPSMEFTd6.cpp.

13099 {
13100  return muVH(sqrt_s) * BrHmumuRatio();
13101 
13102 }

◆ muVHtautau()

double NPSMEFTd6::muVHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13134 of file NPSMEFTd6.cpp.

13135 {
13136  return muVH(sqrt_s) * BrHtautauRatio();
13137 
13138 }

◆ muVHWW()

double NPSMEFTd6::muVHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW}\)

Reimplemented from NPbase.

Definition at line 13026 of file NPSMEFTd6.cpp.

13027 {
13028  return muVH(sqrt_s) * BrHWWRatio();
13029 
13030 }

◆ muVHWW2l2v()

double NPSMEFTd6::muVHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13062 of file NPSMEFTd6.cpp.

13063 {
13064  return muVH(sqrt_s) * BrHWW2l2vRatio();
13065 
13066 }

◆ muVHZga()

double NPSMEFTd6::muVHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12918 of file NPSMEFTd6.cpp.

12919 {
12920  return muVH(sqrt_s) * BrHZgaRatio();
12921 
12922 }

◆ muVHZZ()

double NPSMEFTd6::muVHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12954 of file NPSMEFTd6.cpp.

12955 {
12956  return muVH(sqrt_s) * BrHZZRatio();
12957 
12958 }

◆ muVHZZ4l()

double NPSMEFTd6::muVHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{VH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12990 of file NPSMEFTd6.cpp.

12991 {
12992  return muVH(sqrt_s) * BrHZZ4lRatio();
12993 
12994 }

◆ muWH()

double NPSMEFTd6::muWH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH}\)

Reimplemented from NPbase.

Definition at line 7188 of file NPSMEFTd6.cpp.

7189 {
7190  double mu = 1.0;
7191 
7192  double C1 = 0.0;
7193 
7194  if (sqrt_s == 1.96) {
7195 
7196  C1 = 0.0; // N.A.
7197 
7198  mu +=
7199  +121173. * (1. + eWH_2_Hbox ) * CiHbox / LambdaNP2
7200  +1566788. * (1. + eWH_2_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7201  -160914. * (1. + eWH_2_HD ) * CiHD / LambdaNP2
7202  +860916. * (1. + eWH_2_HW ) * CiHW / LambdaNP2
7203  -286409. * (1. + eWH_2_HWB ) * CiHWB / LambdaNP2
7204  +134641. * (1. + eWH_2_DHW ) * CiDHW / LambdaNP2
7205  -3.31 * (1. + eWH_2_DeltaGF ) * DeltaGF()
7206  -2.199 * deltaMwd6()
7207  ;
7208 
7209  if (FlagQuadraticTerms) {
7210  //Add contributions that are quadratic in the effective coefficients
7211  mu += 0.0;
7212 
7213  }
7214 
7215  } else if (sqrt_s == 7.0) {
7216 
7217  C1 = 0.0106;
7218 
7219  mu +=
7220  +121015. * (1. + eWH_78_Hbox ) * CiHbox / LambdaNP2
7221  +1792020. * (1. + eWH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7222  -159689. * (1. + eWH_78_HD ) * CiHD / LambdaNP2
7223  +881065. * (1. + eWH_78_HW ) * CiHW / LambdaNP2
7224  -283895. * (1. + eWH_78_HWB ) * CiHWB / LambdaNP2
7225  +168173. * (1. + eWH_78_DHW ) * CiDHW / LambdaNP2
7226  -3.273 * (1. + eWH_78_DeltaGF ) * DeltaGF()
7227  -2.143 * deltaMwd6()
7228  ;
7229 
7230  if (FlagQuadraticTerms) {
7231  //Add contributions that are quadratic in the effective coefficients
7232  mu += 0.0;
7233 
7234  }
7235 
7236  } else if (sqrt_s == 8.0) {
7237 
7238  C1 = 0.0105;
7239 
7240  mu +=
7241  +121226. * (1. + eWH_78_Hbox ) * CiHbox / LambdaNP2
7242  +1830192. * (1. + eWH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7243  -159543. * (1. + eWH_78_HD ) * CiHD / LambdaNP2
7244  +884671. * (1. + eWH_78_HW ) * CiHW / LambdaNP2
7245  -283662. * (1. + eWH_78_HWB ) * CiHWB / LambdaNP2
7246  +174061. * (1. + eWH_78_DHW ) * CiDHW / LambdaNP2
7247  -3.278 * (1. + eWH_78_DeltaGF ) * DeltaGF()
7248  -2.147 * deltaMwd6()
7249  ;
7250 
7251  if (FlagQuadraticTerms) {
7252  //Add contributions that are quadratic in the effective coefficients
7253  mu += 0.0;
7254 
7255  }
7256 
7257  } else if (sqrt_s == 13.0) {
7258 
7259  C1 = 0.0103;
7260 
7261  mu +=
7262  +120439. * (1. + eWH_1314_Hbox ) * CiHbox / LambdaNP2
7263  +1953200. * (1. + eWH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7264  -159847. * (1. + eWH_1314_HD ) * CiHD / LambdaNP2
7265  +892264. * (1. + eWH_1314_HW ) * CiHW / LambdaNP2
7266  -283830. * (1. + eWH_1314_HWB ) * CiHWB / LambdaNP2
7267  +192168. * (1. + eWH_1314_DHW ) * CiDHW / LambdaNP2
7268  -3.269 * (1. + eWH_1314_DeltaGF ) * DeltaGF()
7269  -2.101 * deltaMwd6()
7270  ;
7271 
7272  if (FlagQuadraticTerms) {
7273  //Add contributions that are quadratic in the effective coefficients
7274  mu += 0.0;
7275 
7276  }
7277 
7278  } else if (sqrt_s == 14.0) {
7279 
7280  C1 = 0.0103;
7281 
7282  mu +=
7283  +120284. * (1. + eWH_1314_Hbox ) * CiHbox / LambdaNP2
7284  +1971011. * (1. + eWH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7285  -159830. * (1. + eWH_1314_HD ) * CiHD / LambdaNP2
7286  +893216. * (1. + eWH_1314_HW ) * CiHW / LambdaNP2
7287  -283818. * (1. + eWH_1314_HWB ) * CiHWB / LambdaNP2
7288  +194877. * (1. + eWH_1314_DHW ) * CiDHW / LambdaNP2
7289  -3.272 * (1. + eWH_1314_DeltaGF ) * DeltaGF()
7290  -2.103 * deltaMwd6()
7291  ;
7292 
7293  if (FlagQuadraticTerms) {
7294  //Add contributions that are quadratic in the effective coefficients
7295  mu += 0.0;
7296 
7297  }
7298 
7299  } else if (sqrt_s == 27.0) {
7300 
7301  C1 = 0.0101; // From arXiv: 1902.00134
7302 
7303  mu +=
7304  +120696. * CiHbox / LambdaNP2
7305  +2105646. * CiHQ3_11 / LambdaNP2
7306  -159695. * CiHD / LambdaNP2
7307  +900162. * CiHW / LambdaNP2
7308  -283257. * CiHWB / LambdaNP2
7309  +215592. * CiDHW / LambdaNP2
7310  -3.256 * DeltaGF()
7311  -2.063 * deltaMwd6()
7312  ;
7313 
7314  if (FlagQuadraticTerms) {
7315  //Add contributions that are quadratic in the effective coefficients
7316  mu += 0.0;
7317 
7318  }
7319 
7320  } else if (sqrt_s == 100.0) {
7321 
7322  C1 = 0.0; // N.A.
7323 
7324  mu +=
7325  +121319. * CiHbox / LambdaNP2
7326  +2294991. * CiHQ3_11 / LambdaNP2
7327  -159242. * CiHD / LambdaNP2
7328  +908130. * CiHW / LambdaNP2
7329  -282574. * CiHWB / LambdaNP2
7330  +245406. * CiDHW / LambdaNP2
7331  -3.259 * DeltaGF()
7332  -2.047 * deltaMwd6()
7333  ;
7334 
7335  if (FlagQuadraticTerms) {
7336  //Add contributions that are quadratic in the effective coefficients
7337  mu += 0.0;
7338 
7339  }
7340 
7341  } else
7342  throw std::runtime_error("Bad argument in NPSMEFTd6::muWH()");
7343 
7344  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7345  mu += eWHint + eWHpar;
7346 
7347 // Linear contribution from Higgs self-coupling
7348  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
7349 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
7351 
7352  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7353 
7354  return mu;
7355 }

◆ muWHbb()

double NPSMEFTd6::muWHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,bb}\)

Reimplemented from NPbase.

Definition at line 13164 of file NPSMEFTd6.cpp.

13165 {
13166  return muWH(sqrt_s) * BrHbbRatio();
13167 
13168 }

◆ muWHgaga()

double NPSMEFTd6::muWHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12876 of file NPSMEFTd6.cpp.

12877 {
12878  return muWH(sqrt_s) * BrHgagaRatio();
12879 
12880 }

◆ muWHmumu()

double NPSMEFTd6::muWHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13092 of file NPSMEFTd6.cpp.

13093 {
13094  return muWH(sqrt_s) * BrHmumuRatio();
13095 
13096 }

◆ muWHtautau()

double NPSMEFTd6::muWHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13128 of file NPSMEFTd6.cpp.

13129 {
13130  return muWH(sqrt_s) * BrHtautauRatio();
13131 
13132 }

◆ muWHWW()

double NPSMEFTd6::muWHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW}\)

Reimplemented from NPbase.

Definition at line 13020 of file NPSMEFTd6.cpp.

13021 {
13022  return muWH(sqrt_s) * BrHWWRatio();
13023 
13024 }

◆ muWHWW2l2v()

double NPSMEFTd6::muWHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13056 of file NPSMEFTd6.cpp.

13057 {
13058  return muWH(sqrt_s) * BrHWW2l2vRatio();
13059 
13060 }

◆ muWHZga()

double NPSMEFTd6::muWHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12912 of file NPSMEFTd6.cpp.

12913 {
12914  return muWH(sqrt_s) * BrHZgaRatio();
12915 
12916 }

◆ muWHZZ()

double NPSMEFTd6::muWHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12948 of file NPSMEFTd6.cpp.

12949 {
12950  return muWH(sqrt_s) * BrHZZRatio();
12951 
12952 }

◆ muWHZZ4l()

double NPSMEFTd6::muWHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{WH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12984 of file NPSMEFTd6.cpp.

12985 {
12986  return muWH(sqrt_s) * BrHZZ4lRatio();
12987 
12988 }

◆ muZH()

double NPSMEFTd6::muZH ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH}\)

Reimplemented from NPbase.

Definition at line 7357 of file NPSMEFTd6.cpp.

7358 {
7359  double mu = 1.0;
7360 
7361  double C1 = 0.0;
7362 
7363  if (sqrt_s == 1.96) {
7364 
7365  C1 = 0.0; // N.A.
7366 
7367  mu +=
7368  +121197. * (1. + eZH_2_Hbox ) * CiHbox / LambdaNP2
7369  -810445. * (1. + eZH_2_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7370  +529340. * (1. + eZH_2_Hu_11 ) * CiHu_11 / LambdaNP2
7371  -69410.3 * (1. + eZH_2_Hd_11 ) * CiHd_11 / LambdaNP2
7372  +1567161. * (1. + eZH_2_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7373  -16992.5 * (1. + eZH_2_HD ) * CiHD / LambdaNP2
7374  +79314.5 * (1. + eZH_2_HB ) * CiHB / LambdaNP2
7375  +711710. * (1. + eZH_2_HW ) * CiHW / LambdaNP2
7376  +189054. * (1. + eZH_2_HWB ) * CiHWB / LambdaNP2
7377  +9774.73 * (1. + eZH_2_DHB ) * CiDHB / LambdaNP2
7378  +130777. * (1. + eZH_2_DHW ) * CiDHW / LambdaNP2
7379  -2.535 * (1. + eZH_2_DeltaGF ) * DeltaGF()
7380  ;
7381 
7382  if (FlagQuadraticTerms) {
7383  //Add contributions that are quadratic in the effective coefficients
7384  mu += 0.0;
7385 
7386  }
7387 
7388  } else if (sqrt_s == 7.0) {
7389 
7390  C1 = 0.0123;
7391 
7392  mu +=
7393  +121069. * (1. + eZH_78_Hbox ) * CiHbox / LambdaNP2
7394  -182215. * (1. + eZH_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7395  +421780. * (1. + eZH_78_Hu_11 ) * CiHu_11 / LambdaNP2
7396  -139169. * (1. + eZH_78_Hd_11 ) * CiHd_11 / LambdaNP2
7397  +1712111. * (1. + eZH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7398  -15395.4 * (1. + eZH_78_HD ) * CiHD / LambdaNP2
7399  +87094.9 * (1. + eZH_78_HB ) * CiHB / LambdaNP2
7400  +717388. * (1. + eZH_78_HW ) * CiHW / LambdaNP2
7401  +203105. * (1. + eZH_78_HWB ) * CiHWB / LambdaNP2
7402  +17532.4 * (1. + eZH_78_DHB ) * CiDHB / LambdaNP2
7403  +152950. * (1. + eZH_78_DHW ) * CiDHW / LambdaNP2
7404  -2.502 * (1. + eZH_78_DeltaGF ) * DeltaGF()
7405  ;
7406 
7407  if (FlagQuadraticTerms) {
7408  //Add contributions that are quadratic in the effective coefficients
7409  mu += 0.0;
7410 
7411  }
7412 
7413  } else if (sqrt_s == 8.0) {
7414 
7415  C1 = 0.0122;
7416 
7417  mu +=
7418  +121334. * (1. + eZH_78_Hbox ) * CiHbox / LambdaNP2
7419  -176804. * (1. + eZH_78_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7420  +428587. * (1. + eZH_78_Hu_11 ) * CiHu_11 / LambdaNP2
7421  -142508. * (1. + eZH_78_Hd_11 ) * CiHd_11 / LambdaNP2
7422  +1747367. * (1. + eZH_78_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7423  -15002.7 * (1. + eZH_78_HD ) * CiHD / LambdaNP2
7424  +87781.5 * (1. + eZH_78_HB ) * CiHB / LambdaNP2
7425  +721405. * (1. + eZH_78_HW ) * CiHW / LambdaNP2
7426  +204540. * (1. + eZH_78_HWB ) * CiHWB / LambdaNP2
7427  +18868.6 * (1. + eZH_78_DHB ) * CiDHB / LambdaNP2
7428  +158432. * (1. + eZH_78_DHW ) * CiDHW / LambdaNP2
7429  -2.507 * (1. + eZH_78_DeltaGF ) * DeltaGF()
7430  ;
7431 
7432  if (FlagQuadraticTerms) {
7433  //Add contributions that are quadratic in the effective coefficients
7434  mu += 0.0;
7435 
7436  }
7437 
7438  } else if (sqrt_s == 13.0) {
7439 
7440  C1 = 0.0119;
7441 
7442  mu +=
7443  +121374. * (1. + eZH_1314_Hbox ) * CiHbox / LambdaNP2
7444  -152273. * (1. + eZH_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7445  +448168. * (1. + eZH_1314_Hu_11 ) * CiHu_11 / LambdaNP2
7446  -155999. * (1. + eZH_1314_Hd_11 ) * CiHd_11 / LambdaNP2
7447  +1862364. * (1. + eZH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7448  -15185. * (1. + eZH_1314_HD ) * CiHD / LambdaNP2
7449  +88937.9 * (1. + eZH_1314_HB ) * CiHB / LambdaNP2
7450  +728207. * (1. + eZH_1314_HW ) * CiHW / LambdaNP2
7451  +207857. * (1. + eZH_1314_HWB ) * CiHWB / LambdaNP2
7452  +21647.4 * (1. + eZH_1314_DHB ) * CiDHB / LambdaNP2
7453  +175015. * (1. + eZH_1314_DHW ) * CiDHW / LambdaNP2
7454  -2.506 * (1. + eZH_1314_DeltaGF ) * DeltaGF()
7455  ;
7456 
7457  if (FlagQuadraticTerms) {
7458  //Add contributions that are quadratic in the effective coefficients
7459  mu += 0.0;
7460 
7461  }
7462 
7463  } else if (sqrt_s == 14.0) {
7464 
7465  C1 = 0.0118;
7466 
7467  mu +=
7468  +121437. * (1. + eZH_1314_Hbox ) * CiHbox / LambdaNP2
7469  -147580. * (1. + eZH_1314_HQ1_11 ) * CiHQ1_11 / LambdaNP2
7470  +450628. * (1. + eZH_1314_Hu_11 ) * CiHu_11 / LambdaNP2
7471  -157625. * (1. + eZH_1314_Hd_11 ) * CiHd_11 / LambdaNP2
7472  +1878132. * (1. + eZH_1314_HQ3_11 ) * CiHQ3_11 / LambdaNP2
7473  -15299.4 * (1. + eZH_1314_HD ) * CiHD / LambdaNP2
7474  +88761.8 * (1. + eZH_1314_HB ) * CiHB / LambdaNP2
7475  +729243. * (1. + eZH_1314_HW ) * CiHW / LambdaNP2
7476  +207707. * (1. + eZH_1314_HWB ) * CiHWB / LambdaNP2
7477  +21958.9 * (1. + eZH_1314_DHB ) * CiDHB / LambdaNP2
7478  +177300. * (1. + eZH_1314_DHW ) * CiDHW / LambdaNP2
7479  -2.507 * (1. + eZH_1314_DeltaGF ) * DeltaGF()
7480  ;
7481 
7482  if (FlagQuadraticTerms) {
7483  //Add contributions that are quadratic in the effective coefficients
7484  mu += 0.0;
7485 
7486  }
7487 
7488  } else if (sqrt_s == 27.0) {
7489 
7490  C1 = 0.0116; // From arXiv: 1902.00134
7491 
7492  mu +=
7493  +121206. * CiHbox / LambdaNP2
7494  -101865. * CiHQ1_11 / LambdaNP2
7495  +468029. * CiHu_11 / LambdaNP2
7496  -173377. * CiHd_11 / LambdaNP2
7497  +2002478. * CiHQ3_11 / LambdaNP2
7498  -15486.3 * CiHD / LambdaNP2
7499  +89958. * CiHB / LambdaNP2
7500  +735013. * CiHW / LambdaNP2
7501  +211026. * CiHWB / LambdaNP2
7502  +25604. * CiDHB / LambdaNP2
7503  +196710. * CiDHW / LambdaNP2
7504  -2.505 * DeltaGF()
7505  ;
7506 
7507  if (FlagQuadraticTerms) {
7508  //Add contributions that are quadratic in the effective coefficients
7509  mu += 0.0;
7510 
7511  }
7512 
7513  } else if (sqrt_s == 100.0) {
7514 
7515  C1 = 0.0; // N.A.
7516 
7517  mu +=
7518  +121269. * CiHbox / LambdaNP2
7519  +90.68 * CiHQ1_11 / LambdaNP2
7520  +484275. * CiHu_11 / LambdaNP2
7521  -197878. * CiHd_11 / LambdaNP2
7522  +2175601. * CiHQ3_11 / LambdaNP2
7523  -14992.4 * CiHD / LambdaNP2
7524  +91707.3 * CiHB / LambdaNP2
7525  +741805. * CiHW / LambdaNP2
7526  +215319. * CiHWB / LambdaNP2
7527  +31435.6 * CiDHB / LambdaNP2
7528  +223843. * CiDHW / LambdaNP2
7529  -2.504 * DeltaGF()
7530  ;
7531 
7532  if (FlagQuadraticTerms) {
7533  //Add contributions that are quadratic in the effective coefficients
7534  mu += 0.0;
7535  }
7536 
7537  } else
7538  throw std::runtime_error("Bad argument in NPSMEFTd6::muZH()");
7539 
7540  //Add intrinsic and parametric relative theory errors (free par). (Assume they are constant in energy.)
7541  mu += eZHint + eZHpar;
7542 
7543 // Linear contribution from Higgs self-coupling
7544  mu = mu + cLHd6*(C1 + 2.0*dZH)*deltaG_hhhRatio();
7545 // Quadratic contribution from Higgs self-coupling: add separately from FlagQuadraticTerms
7547 
7548  if (mu < 0) return std::numeric_limits<double>::quiet_NaN();
7549 
7550  return mu;
7551 }

◆ muZHbb()

double NPSMEFTd6::muZHbb ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,bb}\)

Reimplemented from NPbase.

Definition at line 13158 of file NPSMEFTd6.cpp.

13159 {
13160  return muZH(sqrt_s) * BrHbbRatio();
13161 
13162 }

◆ muZHgaga()

double NPSMEFTd6::muZHgaga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\gamma\gamma}\)

Reimplemented from NPbase.

Definition at line 12870 of file NPSMEFTd6.cpp.

12871 {
12872  return muZH(sqrt_s) * BrHgagaRatio();
12873 
12874 }

◆ muZHmumu()

double NPSMEFTd6::muZHmumu ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\mu\mu}\)

Reimplemented from NPbase.

Definition at line 13086 of file NPSMEFTd6.cpp.

13087 {
13088  return muZH(sqrt_s) * BrHmumuRatio();
13089 
13090 }

◆ muZHtautau()

double NPSMEFTd6::muZHtautau ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,\tau\tau}\)

Reimplemented from NPbase.

Definition at line 13122 of file NPSMEFTd6.cpp.

13123 {
13124  return muZH(sqrt_s) * BrHtautauRatio();
13125 
13126 }

◆ muZHWW()

double NPSMEFTd6::muZHWW ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW}\)

Reimplemented from NPbase.

Definition at line 13014 of file NPSMEFTd6.cpp.

13015 {
13016  return muZH(sqrt_s) * BrHWWRatio();
13017 
13018 }

◆ muZHWW2l2v()

double NPSMEFTd6::muZHWW2l2v ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,WW\to 2l2\nu}\)

Reimplemented from NPbase.

Definition at line 13050 of file NPSMEFTd6.cpp.

13051 {
13052  return muZH(sqrt_s) * BrHWW2l2vRatio();
13053 
13054 }

◆ muZHZga()

double NPSMEFTd6::muZHZga ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,Z\gamma}\)

Reimplemented from NPbase.

Definition at line 12906 of file NPSMEFTd6.cpp.

12907 {
12908  return muZH(sqrt_s) * BrHZgaRatio();
12909 
12910 }

◆ muZHZZ()

double NPSMEFTd6::muZHZZ ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ}\)

Reimplemented from NPbase.

Definition at line 12942 of file NPSMEFTd6.cpp.

12943 {
12944  return muZH(sqrt_s) * BrHZZRatio();
12945 
12946 }

◆ muZHZZ4l()

double NPSMEFTd6::muZHZZ4l ( const double  sqrt_s) const
virtual

The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.

Parameters
[in]sqrt_sthe center-of-mass energy in TeV
Returns
\(\mu_{ZH,ZZ\to 4l}\)

Reimplemented from NPbase.

Definition at line 12978 of file NPSMEFTd6.cpp.

12979 {
12980  return muZH(sqrt_s) * BrHZZ4lRatio();
12981 
12982 }

◆ Mw()

double NPSMEFTd6::Mw ( ) const
virtual

The mass of the \(W\) boson, \(M_W\).

Returns
\(M_W\) in GeV

Reimplemented from NPbase.

Definition at line 3067 of file NPSMEFTd6.cpp.

3068 {
3069  return (trueSM.Mw() - Mw_tree() / 4.0 / (cW2_tree - sW2_tree)
3070  *(4.0 * sW_tree * cW_tree * CiHWB * v2_over_LambdaNP2
3072  + 2.0 * sW2_tree * DeltaGF()));
3073 }

◆ obliqueS()

double NPSMEFTd6::obliqueS ( ) const
virtual

The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).)

Returns
the value of \(S\)

Reimplemented from NPbase.

Definition at line 2927 of file NPSMEFTd6.cpp.

2928 {
2929  return (4.0 * sW_tree * cW_tree * CiHWB / alphaMz() * v2_over_LambdaNP2);
2930 }

◆ obliqueT()

double NPSMEFTd6::obliqueT ( ) const
virtual

The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).)

Returns
the value of \(T\)

Reimplemented from NPbase.

Definition at line 2932 of file NPSMEFTd6.cpp.

2933 {
2934  return (-CiHD / 2.0 / alphaMz() * v2_over_LambdaNP2);
2935 }

◆ obliqueU()

double NPSMEFTd6::obliqueU ( ) const
virtual

The oblique parameter \(U\).

Returns
the value of \(U\)

Reimplemented from NPbase.

Definition at line 2937 of file NPSMEFTd6.cpp.

2938 {
2939  return 0.0;
2940 }

◆ obliqueW()

double NPSMEFTd6::obliqueW ( ) const
virtual

The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).)

Returns
the value of \(W\)

Reimplemented from NPbase.

Definition at line 2942 of file NPSMEFTd6.cpp.

2943 {
2944  return (- g2_tree * g2_tree * (C2W + 0.5 * C2WS) * v2_over_LambdaNP2 / 2.0);
2945 }

◆ obliqueY()

double NPSMEFTd6::obliqueY ( ) const
virtual

The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).)

Returns
the value of \(Y\)

Reimplemented from NPbase.

Definition at line 2947 of file NPSMEFTd6.cpp.

2948 {
2949  return (- g2_tree * g2_tree * (C2B + 0.5 * C2BS) * v2_over_LambdaNP2 / 2.0);
2950 }

◆ PostUpdate()

bool NPSMEFTd6::PostUpdate ( )
virtual

The post-update method for NPSMEFTd6.

This method runs all the procedures that are need to be executed after the model is successfully updated.

Returns
a boolean that is true if the execution is successful

Reimplemented from NPbase.

Definition at line 957 of file NPSMEFTd6.cpp.

958 {
959  if (!NPbase::PostUpdate()) return (false);
960 
961 // 0) Post-update operations not involving SM nor NP parameters
962  if (!FlagHiggsSM) {
963  cHSM = 0.0;
964  } else {
965  cHSM = 1.0;
966  }
967 
968  if (!FlagLoopHd6) {
969  cLHd6 = 0.0;
970  } else {
971  cLHd6 = 1.0;
972  }
973 
975  cLH3d62 = 1.0;
976  } else {
977  cLH3d62 = 0.0;
978  }
979 
980 // 1) Post-update operations involving SM parameters only
982  v2 = v() * v();
984  aleMz = alphaMz();
985  eeMz = sqrt( 4.0 * M_PI * aleMz );
986  eeMz2 = eeMz*eeMz;
987  cW_tree = Mw_tree() / Mz;
989  sW2_tree = 1.0 - cW2_tree;
990  sW_tree = sqrt(sW2_tree);
991 
992  g1_tree = eeMz/cW_tree;
993  g2_tree = eeMz/sW_tree;
994  g3_tree = sqrt( 4.0 * M_PI * AlsMz );
995 
996  lambdaH_tree = mHl*mHl/2.0/v2;
997 
999  gZlL = (leptons[ELECTRON].getIsospin()) - (leptons[ELECTRON].getCharge())*sW2_tree;
1000  gZlR = - (leptons[ELECTRON].getCharge()) * sW2_tree;
1001  gZuL = (quarks[UP].getIsospin()) - (quarks[UP].getCharge())*sW2_tree;
1002  gZuR = - (quarks[UP].getCharge()) * sW2_tree;
1003  gZdL = (quarks[DOWN].getIsospin()) - (quarks[DOWN].getCharge())*sW2_tree;
1004  gZdR = - (quarks[DOWN].getCharge()) * sW2_tree;
1005 
1006  UevL = 1.0; // Neglect PMNS effects
1007  VudL = 1.0; // Neglect CKM effects
1008 
1009  Yuke = sqrt(2.) * (leptons[ELECTRON].getMass()) / v();
1010  Yukmu = sqrt(2.) * (leptons[MU].getMass()) / v();
1011  Yuktau = sqrt(2.) * (leptons[TAU].getMass()) / v();
1012  Yuku = sqrt(2.) * (quarks[UP].getMass()) / v();
1013  Yukc = sqrt(2.) * (quarks[CHARM].getMass()) / v();
1014  Yukt = sqrt(2.) * mtpole / v();
1015  Yukd = sqrt(2.) * (quarks[DOWN].getMass()) / v();
1016  Yuks = sqrt(2.) * (quarks[STRANGE].getMass()) / v();
1017  Yukb = sqrt(2.) * (quarks[BOTTOM].getMass()) / v();
1018 
1019  dZH = -(9.0/16.0)*( GF*mHl*mHl/sqrt(2.0)/M_PI/M_PI )*( 2.0*M_PI/3.0/sqrt(3.0) - 1.0 );
1020 
1021 // 2) Post-update operations related to assumptions in the form of the dimension-6 operators
1022 
1023 // Rotated CHW and CHB parameters: Here I need to overwrite the model parameters (There are always 2 on/2 off but need the values of both in output)
1024  if (FlagRotateCHWCHB) {
1027  } else {
1030  }
1031 
1032 // Flavour universality assumptions
1033 
1034 // Initialize the internal Wilson coeffs of the form CfH and CfV from the model parameters
1035  CieH_11r = CeH_11r;
1036  CieH_22r = CeH_22r;
1037  CieH_33r = CeH_33r;
1038 
1039  CiuH_11r = CuH_11r;
1040  CiuH_22r = CuH_22r;
1041  CiuH_33r = CuH_33r;
1042 
1043  CidH_11r = CdH_11r;
1044  CidH_22r = CdH_22r;
1045  CidH_33r = CdH_33r;
1046 
1047  CiuG_11r = CuG_11r;
1048  CiuG_22r = CuG_22r;
1049  CiuG_33r = CuG_33r;
1050 
1051  CiuW_11r = CuW_11r;
1052  CiuW_22r = CuW_22r;
1053  CiuW_33r = CuW_33r;
1054 
1055  CiuB_11r = CuB_11r;
1056  CiuB_22r = CuB_22r;
1057  CiuB_33r = CuB_33r;
1058 
1059 // and depending on the flavour assumptions rewrite the values (but never rewritting the values model parameters)
1060 
1061  if (FlagFlavU3OfX || FlagUnivOfX) {
1062 
1063  if (FlagUnivOfX) {
1064 // All equal to uH_33r
1065  CieH_11r = CuH_33r;
1066  CieH_22r = CuH_33r;
1067  CieH_33r = CuH_33r;
1068 
1069  CiuH_11r = CuH_33r;
1070  CiuH_22r = CuH_33r;
1071  // CiuH_33r = CuH_33r;
1072 
1073  CidH_11r = CuH_33r;
1074  CidH_22r = CuH_33r;
1075  CidH_33r = CuH_33r;
1076 
1077  // Currently OfV are only implemented for u quarks so nothing else is needed to apply universality.
1078  }
1079 
1080 // Proportional to Yukawa interactions Wilson coeff in Warsaw - C=y c - Wilson coeff in model par
1081 
1082  CieH_11r = Yuke * CeH_11r;
1083  CieH_22r = Yukmu * CeH_22r;
1084  CieH_33r = Yuktau * CeH_33r;
1085 
1086  CiuH_11r = Yuku * CuH_11r;
1087  CiuH_22r = Yukc * CuH_22r;
1088  CiuH_33r = Yukt * CuH_33r;
1089 
1090  CidH_11r = Yukd * CdH_11r;
1091  CidH_22r = Yuks * CdH_22r;
1092  CidH_33r = Yukb * CdH_33r;
1093 
1094  CiuG_11r = Yuku * CuG_11r;
1095  CiuG_22r = Yukc * CuG_22r;
1096  CiuG_33r = Yukt * CuG_33r;
1097 
1098  CiuW_11r = Yuku * CuW_11r;
1099  CiuW_22r = Yukc * CuW_22r;
1100  CiuW_33r = Yukt * CuW_33r;
1101 
1102  CiuB_11r = Yuku * CuB_11r;
1103  CiuB_22r = Yukc * CuB_22r;
1104  CiuB_33r = Yukt * CuB_33r;
1105  }
1106 
1107 // C2B, C2W, C2WS, C2BS, CDB, CDW, CT are incorporated by change of basis transformation:
1108 // Write here, before working with the dim 6 interactions,
1109 // the contributions from O2W and O2B to the other operators.
1110 // WARNING: Ignoring contributions to 4 fermion-processes for the moment. IMPORTANT FOR LEP2
1111 
1112 // WARNING (OBSOLETE MESSAGE?): if some of the parameters below, e.g. CHL1_11, are not floating in the fit this will
1113 // create a problem since the value generated below CHL1_11 will propagate to the next iteration
1114 // generating an uncontrolled value of the parameter.
1115 // (This is so because SetParameters is not called for non-floating parameters.)
1116 // Possible fix: Not modify model parameters but save everything into internal replicas
1117 // of each model relevant model par. Those then have to be used in the calculations.
1118 // Comment out the following lines until this is resolved
1119 
1120 // Contributionsfrom C2W, C2B, C2WS, C2BS, CT
1121  CiHL1_11 = CHL1_11 - (g1_tree*g1_tree/2.0) * (C2B + 0.5 * C2BS);
1122  CiHL1_22 = CHL1_22 - (g1_tree*g1_tree/2.0) * (C2B + 0.5 * C2BS);
1123  CiHL1_33 = CHL1_33 - (g1_tree*g1_tree/2.0) * (C2B + 0.5 * C2BS);
1124  CiHL3_11 = CHL3_11 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1125  CiHL3_22 = CHL3_22 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1126  CiHL3_33 = CHL3_33 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1127 
1128  CiHQ1_11 = CHQ1_11 + (g1_tree*g1_tree/6.0) * (C2B + 0.5 * C2BS);
1129  CiHQ1_22 = CHQ1_22 + (g1_tree*g1_tree/6.0) * (C2B + 0.5 * C2BS);
1130  CiHQ1_33 = CHQ1_33 + (g1_tree*g1_tree/6.0) * (C2B + 0.5 * C2BS);
1131  CiHQ3_11 = CHQ3_11 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1132  CiHQ3_22 = CHQ3_22 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1133  CiHQ3_33 = CHQ3_33 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1134 
1135  CiHe_11 = CHe_11 - (g1_tree*g1_tree) * (C2B + 0.5 * C2BS);
1136  CiHe_22 = CHe_22 - (g1_tree*g1_tree) * (C2B + 0.5 * C2BS);
1137  CiHe_33 = CHe_33 - (g1_tree*g1_tree) * (C2B + 0.5 * C2BS);
1138 
1139  CiHu_11 = CHu_11 + (2.0*g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1140  CiHu_22 = CHu_22 + (2.0*g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1141  CiHu_33 = CHu_33 + (2.0*g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1142 
1143  CiHd_11 = CHd_11 - (g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1144  CiHd_22 = CHd_22 - (g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1145  CiHd_33 = CHd_33 - (g1_tree*g1_tree/3.0) * (C2B + 0.5 * C2BS);
1146 
1147  CiW = CW + g2_tree * C2W;
1148 
1149  CiHbox = CHbox - 0.5 * CT + (g1_tree*g1_tree/4.0) * (C2B + 0.5 * C2BS) + (3.0*g2_tree*g2_tree/4.0) * (C2W + 0.5 * C2WS);
1150  CiHD = CHD - 2.0 * CT + (g1_tree*g1_tree/4.0) * (C2B + 0.5 * C2BS);
1151  CiH = CH + (2.0*g2_tree*g2_tree*lambdaH_tree) * (C2W + 0.5 * C2WS);
1152 
1153 // For the CfH I must use CifH = CifH + ... to account for previous operations.
1154 
1155  CieH_11r = CieH_11r + (g2_tree*g2_tree*Yuke) * (C2W + 0.5 * C2WS);
1156  CieH_22r = CieH_22r + (g2_tree*g2_tree*Yukmu) * (C2W + 0.5 * C2WS);
1157  CieH_33r = CieH_33r + (g2_tree*g2_tree*Yuktau) * (C2W + 0.5 * C2WS);
1158 
1159  CiuH_11r = CiuH_11r + (g2_tree*g2_tree*Yuku) * (C2W + 0.5 * C2WS);
1160  CiuH_22r = CiuH_22r + (g2_tree*g2_tree*Yukc) * (C2W + 0.5 * C2WS);
1161  CiuH_33r = CiuH_33r + (g2_tree*g2_tree*Yukt) * (C2W + 0.5 * C2WS);
1162 
1163  CidH_11r = CidH_11r + (g2_tree*g2_tree*Yukd) * (C2W + 0.5 * C2WS);
1164  CidH_22r = CidH_22r + (g2_tree*g2_tree*Yuks) * (C2W + 0.5 * C2WS);
1165  CidH_33r = CidH_33r + (g2_tree*g2_tree*Yukb) * (C2W + 0.5 * C2WS);
1166 
1167  CiLL_1221 = CLL_1221 + (g2_tree*g2_tree/2.0) * (C2W + 0.5 * C2WS);
1168  CiLL_2112 = CiLL_1221;
1169 
1170 // Contributionsfrom CDW, DB
1171  CiHB = CHB + (g1_tree/4.0) * CDB;
1172  CiHW = CHW + (g2_tree/4.0) * CDW;
1173 // CiHWHB_gaga = CHWHB_gaga;
1174 // CiHWHB_gagaorth = CHWHB_gagaorth;
1175  CiDHB = CDHB + CDB;
1176  CiDHW = CDHW + CDW;
1177  CiHWB = CHWB + (1.0/4.0) * ( g1_tree * CDW + g2_tree * CDB );
1178 
1179 // 3) Post-update operations working directly with the dimension six operators
1180 
1185  delta_h = (-CiHD / 4.0 + CiHbox) * v2_over_LambdaNP2;
1186 
1187 // Calculation of some quantities repeteadly used in the code
1188 
1189 // NP corrections to Total Higgs width
1191 
1192  if (FlagQuadraticTerms) {
1194  } else {
1195  dGammaHTotR2 = 0.0;
1196  }
1197 
1198 // Total: to be used in BR functions to check positivity
1200 
1201  // The total theory error in the H width: set to 0.0 for the moment
1203 
1204 // Dimension-6 coefficients used in the STXS parameterization
1205  aiG = 16.0 * M_PI * M_PI * CHG * Mw_tree() * Mw_tree() / g3_tree / g3_tree / LambdaNP2;
1206  ai3G = CG * Mw_tree() * Mw_tree() / g3_tree / g3_tree / g3_tree / LambdaNP2;
1207  ai2G =0.0; // Add
1208  aiT = 2.0 * CiHD * v2_over_LambdaNP2;
1209  aiH = - 2.0 * CiHbox * v2_over_LambdaNP2;
1210  aiWW = 0.0; // Add
1211  aiB = 0.0; // Add
1212  aiHW = CiDHW * Mw_tree() * Mw_tree() / 2.0 / g2_tree / LambdaNP2;
1213  aiHB = CiDHB * Mw_tree() * Mw_tree() / 2.0 / g1_tree / LambdaNP2;
1214  aiA = CiHB * Mw_tree() * Mw_tree() / g1_tree / g1_tree / LambdaNP2;
1215  aiHQ = CiHQ1_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1216  aipHQ = CiHQ3_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1217  aiHL = CiHL1_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1218  aipHL = CiHL3_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP. From HEL Lagrangian. Not in original note
1219  aiHu = CiHu_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1220  aiHd = CiHd_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1221  aiHe = CiHe_11 * v2_over_LambdaNP2; // Valid only for flavour universal NP
1223  aiuG = CiuG_33r * Mw_tree() * Mw_tree() / g3_tree / LambdaNP2 / Yukt / 4.0; // From HEL.fr Lagrangian. Not in original note. Valid only for flavour universal NP
1224 
1225 
1226 // Dim 6 SMEFT matching
1227 
1229 
1230  return (true);
1231 }

◆ ppZHprobe()

double NPSMEFTd6::ppZHprobe ( const double  sqrt_s) const
virtual

The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class.

Returns
\(g_p^Z\)

Reimplemented from NPbase.

Definition at line 14899 of file NPSMEFTd6.cpp.

14900 {
14901 
14902  double gpZ=0.0;
14903 
14904  double ghZuL,ghZdL,ghZuR,ghZdR;
14905 
14906  // In the Warsaw basis the contact interactions are generated only by CHF ops but
14907  // in the modified basis ODHB, ODHW also contribute
14908 
14909  ghZuL = -(eeMz/sW_tree/cW_tree)*(CiHQ1_11 - CiHQ3_11 + g1_tree * (1.0/12.0) * CiDHB - (g2_tree/4.0) * CiDHW) * v2_over_LambdaNP2;
14910  ghZdL = -(eeMz/sW_tree/cW_tree)*(CiHQ1_11 + CiHQ3_11 + g1_tree * (1.0/12.0) * CiDHB + (g2_tree/4.0) * CiDHW) * v2_over_LambdaNP2;
14911  ghZuR = -(eeMz/sW_tree/cW_tree)*(CiHu_11 + g1_tree * (1.0/3.0) * CiDHB) * v2_over_LambdaNP2;
14912  ghZdR = -(eeMz/sW_tree/cW_tree)*(CiHd_11 - g1_tree * (1.0/6.0) * CiDHB) * v2_over_LambdaNP2;
14913 
14914  if (sqrt_s == 14.0) {
14915 
14916  gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
14917 
14918  } else if (sqrt_s == 27.0) {
14919  // Use the same as for 14 TeV for the moment
14920 
14921  gpZ = ghZuL - 0.76 * ghZdL - 0.45 * ghZuR + 0.14 * ghZdR;
14922 
14923  } else if (sqrt_s == 100.0) {
14924 
14925  gpZ = ghZuL - 0.90 * ghZdL - 0.45 * ghZuR + 0.17 * ghZdR;
14926 
14927  } else
14928  throw std::runtime_error("Bad argument in NPSMEFTd6::ppZHprobe()");
14929 
14930 
14931  return gpZ;
14932 
14933 }

◆ setFlag()

bool NPSMEFTd6::setFlag ( const std::string  name,
const bool  value 
)
virtual

A method to set a flag of NPSMEFTd6.

Parameters
[in]namename of a model flag
[in]valuethe boolean to be assigned to the flag specified by name
Returns
a boolean that is true if the execution is successful

Reimplemented from StandardModel.

Definition at line 2701 of file NPSMEFTd6.cpp.

2702 {
2703  bool res = false;
2704  if (name.compare("QuadraticTerms") == 0) {
2705  FlagQuadraticTerms = value;
2706  if(value) setModelLinearized(false);
2707  res = true;
2708  } else if (name.compare("RotateCHWCHB") == 0) {
2709  FlagRotateCHWCHB = value;
2710  res = true;
2711  } else if (name.compare("PartialQFU") == 0) {
2712  FlagPartialQFU = value;
2713  res = true;
2714  } else if (name.compare("FlavU3OfX") == 0) {
2715  FlagFlavU3OfX = value;
2716  res = true;
2717  } else if (name.compare("UnivOfX") == 0) {
2718  FlagUnivOfX = value;
2719  res = true;
2720  } else if (name.compare("HiggsSM") == 0) {
2721  FlagHiggsSM = value;
2722  res = true;
2723  } else if (name.compare("LoopHd6") == 0) {
2724  FlagLoopHd6 = value;
2725  res = true;
2726  } else if (name.compare("LoopH3d6Quad") == 0) {
2727  FlagLoopH3d6Quad = value;
2728  res = true;
2729  } else
2730  res = NPbase::setFlag(name, value);
2731 
2732  return (res);
2733 }

◆ setParameter()

void NPSMEFTd6::setParameter ( const std::string  name,
const double &  value 
)
protectedvirtual

A method to set the value of a parameter of the model.

Parameters
[in]namename of a model parameter
[in]valuethe value to be assigned to the parameter specified by name

Reimplemented from StandardModel.

Definition at line 1233 of file NPSMEFTd6.cpp.

1234 {
1235  if (name.compare("CG") == 0)
1236  CG = value;
1237  else if (name.compare("CW") == 0)
1238  CW = value;
1239  else if (name.compare("C2B") == 0)
1240  C2B = value;
1241  else if (name.compare("C2W") == 0)
1242  C2W = value;
1243  else if (name.compare("C2BS") == 0)
1244  C2BS = value;
1245  else if (name.compare("C2WS") == 0)
1246  C2WS = value;
1247  else if (name.compare("CHG") == 0)
1248  CHG = value;
1249  else if (name.compare("CHW") == 0)
1250  CHW = value;
1251  else if (name.compare("CHB") == 0)
1252  CHB = value;
1253  else if (name.compare("CHWHB_gaga") == 0)
1254  CHWHB_gaga = value;
1255  else if (name.compare("CHWHB_gagaorth") == 0)
1256  CHWHB_gagaorth = value;
1257  else if (name.compare("CDHB") == 0)
1258  CDHB = value;
1259  else if (name.compare("CDHW") == 0)
1260  CDHW = value;
1261  else if (name.compare("CDB") == 0)
1262  CDB = value;
1263  else if (name.compare("CDW") == 0)
1264  CDW = value;
1265  else if (name.compare("CHWB") == 0)
1266  CHWB = value;
1267  else if (name.compare("CHD") == 0)
1268  CHD = value;
1269  else if (name.compare("CT") == 0)
1270  CT = value;
1271  else if (name.compare("CHbox") == 0)
1272  CHbox = value;
1273  else if (name.compare("CH") == 0)
1274  CH = value;
1275  else if (name.compare("CHL1_11") == 0)
1276  CHL1_11 = value;
1277  else if (name.compare("CHL1_12r") == 0)
1278  CHL1_12r = value;
1279  else if (name.compare("CHL1_13r") == 0)
1280  CHL1_13r = value;
1281  else if (name.compare("CHL1_22") == 0)
1282  CHL1_22 = value;
1283  else if (name.compare("CHL1_23r") == 0)
1284  CHL1_23r = value;
1285  else if (name.compare("CHL1_33") == 0)
1286  CHL1_33 = value;
1287  else if (name.compare("CHL1_12i") == 0)
1288  CHL1_12i = value;
1289  else if (name.compare("CHL1_13i") == 0)
1290  CHL1_13i = value;
1291  else if (name.compare("CHL1_23i") == 0)
1292  CHL1_23i = value;
1293  else if (name.compare("CHL1") == 0) {
1294  CHL1_11 = value;
1295  CHL1_12r = 0.0;
1296  CHL1_13r = 0.0;
1297  CHL1_22 = value;
1298  CHL1_23r = 0.0;
1299  CHL1_33 = value;
1300  CHL1_12i = 0.0;
1301  CHL1_13i = 0.0;
1302  CHL1_23i = 0.0;
1303  } else if (name.compare("CHL3_11") == 0)
1304  CHL3_11 = value;
1305  else if (name.compare("CHL3_12r") == 0)
1306  CHL3_12r = value;
1307  else if (name.compare("CHL3_13r") == 0)
1308  CHL3_13r = value;
1309  else if (name.compare("CHL3_22") == 0)
1310  CHL3_22 = value;
1311  else if (name.compare("CHL3_23r") == 0)
1312  CHL3_23r = value;
1313  else if (name.compare("CHL3_33") == 0)
1314  CHL3_33 = value;
1315  else if (name.compare("CHL3_12i") == 0)
1316  CHL3_12i = value;
1317  else if (name.compare("CHL3_13i") == 0)
1318  CHL3_13i = value;
1319  else if (name.compare("CHL3_23i") == 0)
1320  CHL3_23i = value;
1321  else if (name.compare("CHL3") == 0) {
1322  CHL3_11 = value;
1323  CHL3_12r = 0.0;
1324  CHL3_13r = 0.0;
1325  CHL3_22 = value;
1326  CHL3_23r = 0.0;
1327  CHL3_33 = value;
1328  CHL3_12i = 0.0;
1329  CHL3_13i = 0.0;
1330  CHL3_23i = 0.0;
1331  } else if (name.compare("CHe_11") == 0)
1332  CHe_11 = value;
1333  else if (name.compare("CHe_12r") == 0)
1334  CHe_12r = value;
1335  else if (name.compare("CHe_13r") == 0)
1336  CHe_13r = value;
1337  else if (name.compare("CHe_22") == 0)
1338  CHe_22 = value;
1339  else if (name.compare("CHe_23r") == 0)
1340  CHe_23r = value;
1341  else if (name.compare("CHe_33") == 0)
1342  CHe_33 = value;
1343  else if (name.compare("CHe_12i") == 0)
1344  CHe_12i = value;
1345  else if (name.compare("CHe_13i") == 0)
1346  CHe_13i = value;
1347  else if (name.compare("CHe_23i") == 0)
1348  CHe_23i = value;
1349  else if (name.compare("CHe") == 0) {
1350  CHe_11 = value;
1351  CHe_12r = 0.0;
1352  CHe_13r = 0.0;
1353  CHe_22 = value;
1354  CHe_23r = 0.0;
1355  CHe_33 = value;
1356  CHe_12i = 0.0;
1357  CHe_13i = 0.0;
1358  CHe_23i = 0.0;
1359  } else if (name.compare("CHQ1_11") == 0) {
1360  CHQ1_11 = value;
1361  if (FlagPartialQFU){
1362  CHQ1_22 = value;
1363  }
1364  } else if (name.compare("CHQ1_12r") == 0)
1365  CHQ1_12r = value;
1366  else if (name.compare("CHQ1_13r") == 0)
1367  CHQ1_13r = value;
1368  else if (name.compare("CHQ1_22") == 0) {
1369  if (!FlagPartialQFU){
1370  CHQ1_22 = value;
1371  }
1372  } else if (name.compare("CHQ1_23r") == 0)
1373  CHQ1_23r = value;
1374  else if (name.compare("CHQ1_33") == 0)
1375  CHQ1_33 = value;
1376  else if (name.compare("CHQ1_12i") == 0)
1377  CHQ1_12i = value;
1378  else if (name.compare("CHQ1_13i") == 0)
1379  CHQ1_13i = value;
1380  else if (name.compare("CHQ1_23i") == 0)
1381  CHQ1_23i = value;
1382  else if (name.compare("CHQ1") == 0) {
1383  CHQ1_11 = value;
1384  CHQ1_12r = 0.0;
1385  CHQ1_13r = 0.0;
1386  CHQ1_22 = value;
1387  CHQ1_23r = 0.0;
1388  CHQ1_33 = value;
1389  CHQ1_12i = 0.0;
1390  CHQ1_13i = 0.0;
1391  CHQ1_23i = 0.0;
1392  } else if (name.compare("CHQ3_11") == 0){
1393  CHQ3_11 = value;
1394  if (FlagPartialQFU){
1395  CHQ3_22 = value;
1396  }
1397  } else if (name.compare("CHQ3_12r") == 0)
1398  CHQ3_12r = value;
1399  else if (name.compare("CHQ3_13r") == 0)
1400  CHQ3_13r = value;
1401  else if (name.compare("CHQ3_22") == 0){
1402  if (!FlagPartialQFU){
1403  CHQ3_22 = value;
1404  }
1405  } else if (name.compare("CHQ3_23r") == 0)
1406  CHQ3_23r = value;
1407  else if (name.compare("CHQ3_33") == 0)
1408  CHQ3_33 = value;
1409  else if (name.compare("CHQ3_12i") == 0)
1410  CHQ3_12i = value;
1411  else if (name.compare("CHQ3_13i") == 0)
1412  CHQ3_13i = value;
1413  else if (name.compare("CHQ3_23i") == 0)
1414  CHQ3_23i = value;
1415  else if (name.compare("CHQ3") == 0) {
1416  CHQ3_11 = value;
1417  CHQ3_12r = 0.0;
1418  CHQ3_13r = 0.0;
1419  CHQ3_22 = value;
1420  CHQ3_23r = 0.0;
1421  CHQ3_33 = value;
1422  CHQ3_12i = 0.0;
1423  CHQ3_13i = 0.0;
1424  CHQ3_23i = 0.0;
1425  } else if (name.compare("CHu_11") == 0){
1426  CHu_11 = value;
1427  if (FlagPartialQFU){
1428  CHu_22 = value;
1429  }
1430  } else if (name.compare("CHu_12r") == 0)
1431  CHu_12r = value;
1432  else if (name.compare("CHu_13r") == 0)
1433  CHu_13r = value;
1434  else if (name.compare("CHu_22") == 0){
1435  if (!FlagPartialQFU){
1436  CHu_22 = value;
1437  }
1438  } else if (name.compare("CHu_23r") == 0)
1439  CHu_23r = value;
1440  else if (name.compare("CHu_33") == 0)
1441  CHu_33 = value;
1442  else if (name.compare("CHu_12i") == 0)
1443  CHu_12i = value;
1444  else if (name.compare("CHu_13i") == 0)
1445  CHu_13i = value;
1446  else if (name.compare("CHu_23i") == 0)
1447  CHu_23i = value;
1448  else if (name.compare("CHu") == 0) {
1449  CHu_11 = value;
1450  CHu_12r = 0.0;
1451  CHu_13r = 0.0;
1452  CHu_22 = value;
1453  CHu_23r = 0.0;
1454  CHu_33 = value;
1455  CHu_12i = 0.0;
1456  CHu_13i = 0.0;
1457  CHu_23i = 0.0;
1458  } else if (name.compare("CHd_11") == 0){
1459  CHd_11 = value;
1460  if (FlagPartialQFU){
1461  CHd_22 = value;
1462  }
1463  } else if (name.compare("CHd_12r") == 0)
1464  CHd_12r = value;
1465  else if (name.compare("CHd_13r") == 0)
1466  CHd_13r = value;
1467  else if (name.compare("CHd_22") == 0){
1468  if (!FlagPartialQFU){
1469  CHd_22 = value;
1470  }
1471  } else if (name.compare("CHd_23r") == 0)
1472  CHd_23r = value;
1473  else if (name.compare("CHd_33") == 0)
1474  CHd_33 = value;
1475  else if (name.compare("CHd_12i") == 0)
1476  CHd_12i = value;
1477  else if (name.compare("CHd_13i") == 0)
1478  CHd_13i = value;
1479  else if (name.compare("CHd_23i") == 0)
1480  CHd_23i = value;
1481  else if (name.compare("CHd") == 0) {
1482  CHd_11 = value;
1483  CHd_12r = 0.0;
1484  CHd_13r = 0.0;
1485  CHd_22 = value;
1486  CHd_23r = 0.0;
1487  CHd_33 = value;
1488  CHd_12i = 0.0;
1489  CHd_13i = 0.0;
1490  CHd_23i = 0.0;
1491  } else if (name.compare("CHud_11r") == 0){
1492  CHud_11r = value;
1493  if (FlagPartialQFU){
1494  CHud_22r = value;
1495  }
1496  } else if (name.compare("CHud_12r") == 0)
1497  CHud_12r = value;
1498  else if (name.compare("CHud_13r") == 0)
1499  CHud_13r = value;
1500  else if (name.compare("CHud_22r") == 0){
1501  if (!FlagPartialQFU){
1502  CHud_22r = value;
1503  }
1504  } else if (name.compare("CHud_23r") == 0)
1505  CHud_23r = value;
1506  else if (name.compare("CHud_33r") == 0)
1507  CHud_33r = value;
1508  else if (name.compare("CHud_r") == 0) {
1509  CHud_11r = value;
1510  CHud_12r = 0.0;
1511  CHud_13r = 0.0;
1512  CHud_22r = value;
1513  CHud_23r = 0.0;
1514  CHud_33r = value;
1515  } else if (name.compare("CHud_11i") == 0){
1516  CHud_11i = value;
1517  if (FlagPartialQFU){
1518  CHud_22i = value;
1519  }
1520  } else if (name.compare("CHud_12i") == 0)
1521  CHud_12i = value;
1522  else if (name.compare("CHud_13i") == 0)
1523  CHud_13i = value;
1524  else if (name.compare("CHud_22i") == 0){
1525  if (!FlagPartialQFU){
1526  CHud_22i = value;
1527  }
1528  } else if (name.compare("CHud_23i") == 0)
1529  CHud_23i = value;
1530  else if (name.compare("CHud_33i") == 0)
1531  CHud_33i = value;
1532  else if (name.compare("CHud_i") == 0) {
1533  CHud_11i = value;
1534  CHud_12i = 0.0;
1535  CHud_13i = 0.0;
1536  CHud_22i = value;
1537  CHud_23i = 0.0;
1538  CHud_33i = value;
1539  } else if (name.compare("CeH_11r") == 0){
1540  if (!FlagFlavU3OfX){
1541  CeH_11r = value;
1542  }
1543  } else if (name.compare("CeH_12r") == 0)
1544  CeH_12r = value;
1545  else if (name.compare("CeH_13r") == 0)
1546  CeH_13r = value;
1547  else if (name.compare("CeH_22r") == 0){
1548  if (!FlagFlavU3OfX){
1549  CeH_22r = value;
1550  }
1551  } else if (name.compare("CeH_23r") == 0)
1552  CeH_23r = value;
1553  else if (name.compare("CeH_33r") == 0){
1554  CeH_33r = value;
1555  if (FlagFlavU3OfX){
1556  CeH_11r = value;
1557  CeH_22r = value;
1558  }
1559  } else if (name.compare("CeH_11i") == 0)
1560  CeH_11i = value;
1561  else if (name.compare("CeH_12i") == 0)
1562  CeH_12i = value;
1563  else if (name.compare("CeH_13i") == 0)
1564  CeH_13i = value;
1565  else if (name.compare("CeH_22i") == 0)
1566  CeH_22i = value;
1567  else if (name.compare("CeH_23i") == 0)
1568  CeH_23i = value;
1569  else if (name.compare("CeH_33i") == 0)
1570  CeH_33i = value;
1571  else if (name.compare("CuH_11r") == 0){
1572  if (!FlagFlavU3OfX){
1573  CuH_11r = value;
1574  }
1575  } else if (name.compare("CuH_12r") == 0)
1576  CuH_12r = value;
1577  else if (name.compare("CuH_13r") == 0)
1578  CuH_13r = value;
1579  else if (name.compare("CuH_22r") == 0){
1580  if (!FlagFlavU3OfX){
1581  CuH_22r = value;
1582  }
1583  } else if (name.compare("CuH_23r") == 0)
1584  CuH_23r = value;
1585  else if (name.compare("CuH_33r") == 0){
1586  CuH_33r = value;
1587  if (FlagFlavU3OfX){
1588  CuH_11r = value;
1589  CuH_22r = value;
1590  }
1591  } else if (name.compare("CuH_11i") == 0)
1592  CuH_11i = value;
1593  else if (name.compare("CuH_12i") == 0)
1594  CuH_12i = value;
1595  else if (name.compare("CuH_13i") == 0)
1596  CuH_13i = value;
1597  else if (name.compare("CuH_22i") == 0)
1598  CuH_22i = value;
1599  else if (name.compare("CuH_23i") == 0)
1600  CuH_23i = value;
1601  else if (name.compare("CuH_33i") == 0)
1602  CuH_33i = value;
1603  else if (name.compare("CdH_11r") == 0){
1604  if (!FlagFlavU3OfX){
1605  CdH_11r = value;
1606  }
1607  } else if (name.compare("CdH_12r") == 0)
1608  CdH_12r = value;
1609  else if (name.compare("CdH_13r") == 0)
1610  CdH_13r = value;
1611  else if (name.compare("CdH_22r") == 0){
1612  if (!FlagFlavU3OfX){
1613  CdH_22r = value;
1614  }
1615  } else if (name.compare("CdH_23r") == 0)
1616  CdH_23r = value;
1617  else if (name.compare("CdH_33r") == 0){
1618  CdH_33r = value;
1619  if (FlagFlavU3OfX){
1620  CdH_11r = value;
1621  CdH_22r = value;
1622  }
1623  } else if (name.compare("CdH_11i") == 0)
1624  CdH_11i = value;
1625  else if (name.compare("CdH_12i") == 0)
1626  CdH_12i = value;
1627  else if (name.compare("CdH_13i") == 0)
1628  CdH_13i = value;
1629  else if (name.compare("CdH_22i") == 0)
1630  CdH_22i = value;
1631  else if (name.compare("CdH_23i") == 0)
1632  CdH_23i = value;
1633  else if (name.compare("CdH_33i") == 0)
1634  CdH_33i = value;
1635  else if (name.compare("CuG_11r") == 0){
1636  if (!FlagFlavU3OfX){
1637  CuG_11r = value;
1638  }
1639  } else if (name.compare("CuG_12r") == 0)
1640  CuG_12r = value;
1641  else if (name.compare("CuG_13r") == 0)
1642  CuG_13r = value;
1643  else if (name.compare("CuG_22r") == 0){
1644  if (!FlagFlavU3OfX){
1645  CuG_22r = value;
1646  }
1647  } else if (name.compare("CuG_23r") == 0)
1648  CuG_23r = value;
1649  else if (name.compare("CuG_33r") == 0){
1650  CuG_33r = value;
1651  if (FlagFlavU3OfX){
1652  CuG_11r = value;
1653  CuG_22r = value;
1654  }
1655  } else if (name.compare("CuG_r") == 0) {
1656  CuG_11r = value;
1657  CuG_12r = 0.0;
1658  CuG_13r = 0.0;
1659  CuG_22r = value;
1660  CuG_23r = 0.0;
1661  CuG_33r = value;
1662  } else if (name.compare("CuG_11i") == 0)
1663  CuG_11i = value;
1664  else if (name.compare("CuG_12i") == 0)
1665  CuG_12i = value;
1666  else if (name.compare("CuG_13i") == 0)
1667  CuG_13i = value;
1668  else if (name.compare("CuG_22i") == 0)
1669  CuG_22i = value;
1670  else if (name.compare("CuG_23i") == 0)
1671  CuG_23i = value;
1672  else if (name.compare("CuG_33i") == 0)
1673  CuG_33i = value;
1674  else if (name.compare("CuG_i") == 0) {
1675  CuG_11i = value;
1676  CuG_12i = 0.0;
1677  CuG_13i = 0.0;
1678  CuG_22i = value;
1679  CuG_23i = 0.0;
1680  CuG_33i = value;
1681  } else if (name.compare("CuW_11r") == 0){
1682  if (!FlagFlavU3OfX){
1683  CuW_11r = value;
1684  }
1685  } else if (name.compare("CuW_12r") == 0)
1686  CuW_12r = value;
1687  else if (name.compare("CuW_13r") == 0)
1688  CuW_13r = value;
1689  else if (name.compare("CuW_22r") == 0){
1690  if (!FlagFlavU3OfX){
1691  CuW_22r = value;
1692  }
1693  } else if (name.compare("CuW_23r") == 0)
1694  CuW_23r = value;
1695  else if (name.compare("CuW_33r") == 0){
1696  CuW_33r = value;
1697  if (FlagFlavU3OfX){
1698  CuW_11r = value;
1699  CuW_22r = value;
1700  }
1701  } else if (name.compare("CuW_r") == 0) {
1702  CuW_11r = value;
1703  CuW_12r = 0.0;
1704  CuW_13r = 0.0;
1705  CuW_22r = value;
1706  CuW_23r = 0.0;
1707  CuW_33r = value;
1708  } else if (name.compare("CuW_11i") == 0)
1709  CuW_11i = value;
1710  else if (name.compare("CuW_12i") == 0)
1711  CuW_12i = value;
1712  else if (name.compare("CuW_13i") == 0)
1713  CuW_13i = value;
1714  else if (name.compare("CuW_22i") == 0)
1715  CuW_22i = value;
1716  else if (name.compare("CuW_23i") == 0)
1717  CuW_23i = value;
1718  else if (name.compare("CuW_33i") == 0)
1719  CuW_33i = value;
1720  else if (name.compare("CuW_i") == 0) {
1721  CuW_11i = value;
1722  CuW_12i = 0.0;
1723  CuW_13i = 0.0;
1724  CuW_22i = value;
1725  CuW_23i = 0.0;
1726  CuW_33i = value;
1727  } else if (name.compare("CuB_11r") == 0){
1728  if (!FlagFlavU3OfX){
1729  CuB_11r = value;
1730  }
1731  } else if (name.compare("CuB_12r") == 0)
1732  CuB_12r = value;
1733  else if (name.compare("CuB_13r") == 0)
1734  CuB_13r = value;
1735  else if (name.compare("CuB_22r") == 0){
1736  if (!FlagFlavU3OfX){
1737  CuB_22r = value;
1738  }
1739  } else if (name.compare("CuB_23r") == 0)
1740  CuB_23r = value;
1741  else if (name.compare("CuB_33r") == 0){
1742  CuB_33r = value;
1743  if (FlagFlavU3OfX){
1744  CuB_11r = value;
1745  CuB_22r = value;
1746  }
1747  } else if (name.compare("CuB_r") == 0) {
1748  CuB_11r = value;
1749  CuB_12r = 0.0;
1750  CuB_13r = 0.0;
1751  CuB_22r = value;
1752  CuB_23r = 0.0;
1753  CuB_33r = value;
1754  } else if (name.compare("CuB_11i") == 0)
1755  CuB_11i = value;
1756  else if (name.compare("CuB_12i") == 0)
1757  CuB_12i = value;
1758  else if (name.compare("CuB_13i") == 0)
1759  CuB_13i = value;
1760  else if (name.compare("CuB_22i") == 0)
1761  CuB_22i = value;
1762  else if (name.compare("CuB_23i") == 0)
1763  CuB_23i = value;
1764  else if (name.compare("CuB_33i") == 0)
1765  CuB_33i = value;
1766  else if (name.compare("CuB_i") == 0) {
1767  CuB_11i = value;
1768  CuB_12i = 0.0;
1769  CuB_13i = 0.0;
1770  CuB_22i = value;
1771  CuB_23i = 0.0;
1772  CuB_33i = value;
1773  } else if (name.compare("CdG_11r") == 0){
1774  if (!FlagFlavU3OfX){
1775  CdG_11r = value;
1776  }
1777  } else if (name.compare("CdG_12r") == 0)
1778  CdG_12r = value;
1779  else if (name.compare("CdG_13r") == 0)
1780  CdG_13r = value;
1781  else if (name.compare("CdG_22r") == 0){
1782  if (!FlagFlavU3OfX){
1783  CdG_22r = value;
1784  }
1785  } else if (name.compare("CdG_23r") == 0)
1786  CdG_23r = value;
1787  else if (name.compare("CdG_33r") == 0){
1788  CdG_33r = value;
1789  if (FlagFlavU3OfX){
1790  CdG_11r = value;
1791  CdG_22r = value;
1792  }
1793  } else if (name.compare("CdG_r") == 0) {
1794  CdG_11r = value;
1795  CdG_12r = 0.0;
1796  CdG_13r = 0.0;
1797  CdG_22r = value;
1798  CdG_23r = 0.0;
1799  CdG_33r = value;
1800  } else if (name.compare("CdG_11i") == 0)
1801  CdG_11i = value;
1802  else if (name.compare("CdG_12i") == 0)
1803  CdG_12i = value;
1804  else if (name.compare("CdG_13i") == 0)
1805  CdG_13i = value;
1806  else if (name.compare("CdG_22i") == 0)
1807  CdG_22i = value;
1808  else if (name.compare("CdG_23i") == 0)
1809  CdG_23i = value;
1810  else if (name.compare("CdG_33i") == 0)
1811  CdG_33i = value;
1812  else if (name.compare("CdG_i") == 0) {
1813  CdG_11i = value;
1814  CdG_12i = 0.0;
1815  CdG_13i = 0.0;
1816  CdG_22i = value;
1817  CdG_23i = 0.0;
1818  CdG_33i = value;
1819  } else if (name.compare("CdW_11r") == 0){
1820  if (!FlagFlavU3OfX){
1821  CdW_11r = value;
1822  }
1823  } else if (name.compare("CdW_12r") == 0)
1824  CdW_12r = value;
1825  else if (name.compare("CdW_13r") == 0)
1826  CdW_13r = value;
1827  else if (name.compare("CdW_22r") == 0){
1828  if (!FlagFlavU3OfX){
1829  CdW_22r = value;
1830  }
1831  } else if (name.compare("CdW_23r") == 0)
1832  CdW_23r = value;
1833  else if (name.compare("CdW_33r") == 0){
1834  CdW_33r = value;
1835  if (FlagFlavU3OfX){
1836  CdW_11r = value;
1837  CdW_22r = value;
1838  }
1839  } else if (name.compare("CdW_r") == 0) {
1840  CdW_11r = value;
1841  CdW_12r = 0.0;
1842  CdW_13r = 0.0;
1843  CdW_22r = value;
1844  CdW_23r = 0.0;
1845  CdW_33r = value;
1846  } else if (name.compare("CdW_11i") == 0)
1847  CdW_11i = value;
1848  else if (name.compare("CdW_12i") == 0)
1849  CdW_12i = value;
1850  else if (name.compare("CdW_13i") == 0)
1851  CdW_13i = value;
1852  else if (name.compare("CdW_22i") == 0)
1853  CdW_22i = value;
1854  else if (name.compare("CdW_23i") == 0)
1855  CdW_23i = value;
1856  else if (name.compare("CdW_33i") == 0)
1857  CdW_33i = value;
1858  else if (name.compare("CdW_i") == 0) {
1859  CdW_11i = value;
1860  CdW_12i = 0.0;
1861  CdW_13i = 0.0;
1862  CdW_22i = value;
1863  CdW_23i = 0.0;
1864  CdW_33i = value;
1865  } else if (name.compare("CdB_11r") == 0){
1866  if (!FlagFlavU3OfX){
1867  CdB_11r = value;
1868  }
1869  } else if (name.compare("CdB_12r") == 0)
1870  CdB_12r = value;
1871  else if (name.compare("CdB_13r") == 0)
1872  CdB_13r = value;
1873  else if (name.compare("CdB_22r") == 0){
1874  if (!FlagFlavU3OfX){
1875  CdB_22r = value;
1876  }
1877  } else if (name.compare("CdB_23r") == 0)
1878  CdB_23r = value;
1879  else if (name.compare("CdB_33r") == 0){
1880  CdB_33r = value;
1881  if (FlagFlavU3OfX){
1882  CdB_11r = value;
1883  CdB_22r = value;
1884  }
1885  } else if (name.compare("CdB_r") == 0) {
1886  CdB_11r = value;
1887  CdB_12r = 0.0;
1888  CdB_13r = 0.0;
1889  CdB_22r = value;
1890  CdB_23r = 0.0;
1891  CdB_33r = value;
1892  } else if (name.compare("CdB_11i") == 0)
1893  CdB_11i = value;
1894  else if (name.compare("CdB_12i") == 0)
1895  CdB_12i = value;
1896  else if (name.compare("CdB_13i") == 0)
1897  CdB_13i = value;
1898  else if (name.compare("CdB_22i") == 0)
1899  CdB_22i = value;
1900  else if (name.compare("CdB_23i") == 0)
1901  CdB_23i = value;
1902  else if (name.compare("CdB_33i") == 0)
1903  CdB_33i = value;
1904  else if (name.compare("CdB_i") == 0) {
1905  CdB_11i = value;
1906  CdB_12i = 0.0;
1907  CdB_13i = 0.0;
1908  CdB_22i = value;
1909  CdB_23i = 0.0;
1910  CdB_33i = value;
1911  } else if (name.compare("CeW_11r") == 0){
1912  if (!FlagFlavU3OfX){
1913  CeW_11r = value;
1914  }
1915  } else if (name.compare("CeW_12r") == 0)
1916  CeW_12r = value;
1917  else if (name.compare("CeW_13r") == 0)
1918  CeW_13r = value;
1919  else if (name.compare("CeW_22r") == 0){
1920  if (!FlagFlavU3OfX){
1921  CeW_22r = value;
1922  }
1923  } else if (name.compare("CeW_23r") == 0)
1924  CeW_23r = value;
1925  else if (name.compare("CeW_33r") == 0){
1926  CeW_33r = value;
1927  if (FlagFlavU3OfX){
1928  CeW_11r = value;
1929  CeW_22r = value;
1930  }
1931  } else if (name.compare("CeW_r") == 0) {
1932  CeW_11r = value;
1933  CeW_12r = 0.0;
1934  CeW_13r = 0.0;
1935  CeW_22r = value;
1936  CeW_23r = 0.0;
1937  CeW_33r = value;
1938  } else if (name.compare("CeW_11i") == 0)
1939  CeW_11i = value;
1940  else if (name.compare("CeW_12i") == 0)
1941  CeW_12i = value;
1942  else if (name.compare("CeW_13i") == 0)
1943  CeW_13i = value;
1944  else if (name.compare("CeW_22i") == 0)
1945  CeW_22i = value;
1946  else if (name.compare("CeW_23i") == 0)
1947  CeW_23i = value;
1948  else if (name.compare("CeW_33i") == 0)
1949  CeW_33i = value;
1950  else if (name.compare("CeW_i") == 0) {
1951  CeW_11i = value;
1952  CeW_12i = 0.0;
1953  CeW_13i = 0.0;
1954  CeW_22i = value;
1955  CeW_23i = 0.0;
1956  CeW_33i = value;
1957  } else if (name.compare("CeB_11r") == 0){
1958  if (!FlagFlavU3OfX){
1959  CeB_11r = value;
1960  }
1961  } else if (name.compare("CeB_12r") == 0)
1962  CeB_12r = value;
1963  else if (name.compare("CeB_13r") == 0)
1964  CeB_13r = value;
1965  else if (name.compare("CeB_22r") == 0){
1966  if (!FlagFlavU3OfX){
1967  CeB_22r = value;
1968  }
1969  } else if (name.compare("CeB_23r") == 0)
1970  CeB_23r = value;
1971  else if (name.compare("CeB_33r") == 0){
1972  CeB_33r = value;
1973  if (FlagFlavU3OfX){
1974  CeB_11r = value;
1975  CeB_22r = value;
1976  }
1977  } else if (name.compare("CeB_r") == 0) {
1978  CeB_11r = value;
1979  CeB_12r = 0.0;
1980  CeB_13r = 0.0;
1981  CeB_22r = value;
1982  CeB_23r = 0.0;
1983  CeB_33r = value;
1984  } else if (name.compare("CeB_11i") == 0)
1985  CeB_11i = value;
1986  else if (name.compare("CeB_12i") == 0)
1987  CeB_12i = value;
1988  else if (name.compare("CeB_13i") == 0)
1989  CeB_13i = value;
1990  else if (name.compare("CeB_22i") == 0)
1991  CeB_22i = value;
1992  else if (name.compare("CeB_23i") == 0)
1993  CeB_23i = value;
1994  else if (name.compare("CeB_33i") == 0)
1995  CeB_33i = value;
1996  else if (name.compare("CeB_i") == 0) {
1997  CeB_11i = value;
1998  CeB_12i = 0.0;
1999  CeB_13i = 0.0;
2000  CeB_22i = value;
2001  CeB_23i = 0.0;
2002  CeB_33i = value;
2003 // Several redundancies for the 4-fermionn operators below
2004  } else if (name.compare("CLL_1111") == 0) {
2005  CLL_1111 = value;
2006  } else if (name.compare("CLL_1122") == 0) {
2007  CLL_1122 = value;
2008  CLL_2211 = value;
2009  } else if (name.compare("CLL_1133") == 0) {
2010  CLL_1133 = value;
2011  CLL_3311 = value;
2012  } else if (name.compare("CLL_1221") == 0) {
2013  CLL_1221 = value;
2014  CLL_2112 = value;
2015  } else if (name.compare("CLL_1331") == 0) {
2016  CLL_1331 = value;
2017  CLL_3113 = value;
2018  } else if (name.compare("CLL") == 0) {
2019  CLL_1111 = value;
2020  CLL_1221 = value;
2021  CLL_2112 = value;
2022  CLL_2211 = value;
2023  CLL_1122 = value;
2024  CLL_3311 = value;
2025  CLL_1133 = value;
2026  CLL_1331 = value;
2027  CLL_3113 = value;
2028  } else if (name.compare("CLQ1_1111") == 0) {
2029  CLQ1_1111 = value;
2030  } else if (name.compare("CLQ1_1122") == 0) {
2031  CLQ1_1122 = value;
2032  } else if (name.compare("CLQ1_2211") == 0) {
2033  CLQ1_2211 = value;
2034  } else if (name.compare("CLQ1_2112") == 0) {
2035  CLQ1_2112 = value;
2036  } else if (name.compare("CLQ1_1221") == 0) {
2037  CLQ1_1221 = value;
2038  } else if (name.compare("CLQ1_1133") == 0) {
2039  CLQ1_1133 = value;
2040  } else if (name.compare("CLQ1_3311") == 0) {
2041  CLQ1_3311 = value;
2042  } else if (name.compare("CLQ1_3113") == 0) {
2043  CLQ1_3113 = value;
2044  } else if (name.compare("CLQ1_1331") == 0) {
2045  CLQ1_1331 = value;
2046  } else if (name.compare("CLQ1_1123") == 0) {
2047  CLQ1_1123 = value;
2048  } else if (name.compare("CLQ1_2223") == 0) {
2049  CLQ1_2223 = value;
2050  } else if (name.compare("CLQ1_3323") == 0) {
2051  CLQ1_3323 = value;
2052  } else if (name.compare("CLQ1_1132") == 0) {
2053  CLQ1_1132 = value;
2054  } else if (name.compare("CLQ1_2232") == 0) {
2055  CLQ1_2232 = value;
2056  } else if (name.compare("CLQ1_3332") == 0) {
2057  CLQ1_3332 = value;
2058  } else if (name.compare("CLQ1") == 0) {
2059  CLQ1_1111 = value;
2060  CLQ1_1122 = value;
2061  CLQ1_2211 = value;
2062  CLQ1_1221 = value;
2063  CLQ1_2112 = value;
2064  CLQ1_1133 = value;
2065  CLQ1_3311 = value;
2066  CLQ1_1331 = value;
2067  CLQ1_3113 = value;
2068  } else if (name.compare("CLQ3_1111") == 0) {
2069  CLQ3_1111 = value;
2070  } else if (name.compare("CLQ3_1122") == 0) {
2071  CLQ3_1122 = value;
2072  } else if (name.compare("CLQ3_2211") == 0) {
2073  CLQ3_2211 = value;
2074  } else if (name.compare("CLQ3_2112") == 0) {
2075  CLQ3_2112 = value;
2076  } else if (name.compare("CLQ3_1221") == 0) {
2077  CLQ3_1221 = value;
2078  } else if (name.compare("CLQ3_1133") == 0) {
2079  CLQ3_1133 = value;
2080  } else if (name.compare("CLQ3_3311") == 0) {
2081  CLQ3_3311 = value;
2082  } else if (name.compare("CLQ3_3113") == 0) {
2083  CLQ3_3113 = value;
2084  } else if (name.compare("CLQ3_1331") == 0) {
2085  CLQ3_1331 = value;
2086  } else if (name.compare("CLQ3_1123") == 0) {
2087  CLQ3_1123 = value;
2088  } else if (name.compare("CLQ3_2223") == 0) {
2089  CLQ3_2223 = value;
2090  } else if (name.compare("CLQ3_3323") == 0) {
2091  CLQ3_3323 = value;
2092  } else if (name.compare("CLQ3_1132") == 0) {
2093  CLQ3_1132 = value;
2094  } else if (name.compare("CLQ3_2232") == 0) {
2095  CLQ3_2232 = value;
2096  } else if (name.compare("CLQ3_3332") == 0) {
2097  CLQ3_3332 = value;
2098  } else if (name.compare("CLQ3") == 0) {
2099  CLQ3_1111 = value;
2100  CLQ3_1122 = value;
2101  CLQ3_2211 = value;
2102  CLQ3_1221 = value;
2103  CLQ3_2112 = value;
2104  CLQ3_1133 = value;
2105  CLQ3_3311 = value;
2106  CLQ3_1331 = value;
2107  CLQ3_3113 = value;
2108  } else if (name.compare("Cee") == 0) {
2109  Cee_1111 = value;
2110  Cee_1122 = value;
2111  Cee_2211 = value;
2112  Cee_1133 = value;
2113  Cee_3311 = value;
2114  } else if (name.compare("Cee_1111") == 0) {
2115  Cee_1111 = value;
2116  } else if (name.compare("Cee_1122") == 0) {
2117  Cee_1122 = value;
2118  Cee_2211 = value;
2119  } else if (name.compare("Cee_1133") == 0) {
2120  Cee_1133 = value;
2121  Cee_3311 = value;
2122  } else if (name.compare("Ceu") == 0) {
2123  Ceu_1111 = value;
2124  Ceu_1122 = value;
2125  Ceu_2211 = value;
2126  Ceu_1133 = value;
2127  Ceu_2233 = value;
2128  Ceu_3311 = value;
2129  } else if (name.compare("Ceu_1111") == 0) {
2130  Ceu_1111 = value;
2131  } else if (name.compare("Ceu_1122") == 0) {
2132  Ceu_1122 = value;
2133  } else if (name.compare("Ceu_2211") == 0) {
2134  Ceu_2211 = value;
2135  } else if (name.compare("Ceu_1133") == 0) {
2136  Ceu_1133 = value;
2137  } else if (name.compare("Ceu_2233") == 0) {
2138  Ceu_2233 = value;
2139  } else if (name.compare("Ceu_3311") == 0) {
2140  Ceu_3311 = value;
2141  } else if (name.compare("Ced") == 0) {
2142  Ced_1111 = value;
2143  Ced_1122 = value;
2144  Ced_2211 = value;
2145  Ced_1133 = value;
2146  Ced_3311 = value;
2147  } else if (name.compare("Ced_1111") == 0) {
2148  Ced_1111 = value;
2149  } else if (name.compare("Ced_1122") == 0) {
2150  Ced_1122 = value;
2151  } else if (name.compare("Ced_2211") == 0) {
2152  Ced_2211 = value;
2153  } else if (name.compare("Ced_1133") == 0) {
2154  Ced_1133 = value;
2155  } else if (name.compare("Ced_3311") == 0) {
2156  Ced_3311 = value;
2157  } else if (name.compare("Ced_1123") == 0) {
2158  Ced_1123 = value;
2159  } else if (name.compare("Ced_2223") == 0) {
2160  Ced_2223 = value;
2161  } else if (name.compare("Ced_3323") == 0) {
2162  Ced_3323 = value;
2163  } else if (name.compare("Ced_1132") == 0) {
2164  Ced_1132 = value;
2165  } else if (name.compare("Ced_2232") == 0) {
2166  Ced_2232 = value;
2167  } else if (name.compare("Ced_3332") == 0) {
2168  Ced_3332 = value;
2169  } else if (name.compare("CLe") == 0) {
2170  CLe_1111 = value;
2171  CLe_1122 = value;
2172  CLe_2211 = value;
2173  CLe_1133 = value;
2174  CLe_3311 = value;
2175  } else if (name.compare("CLe_1111") == 0) {
2176  CLe_1111 = value;
2177  } else if (name.compare("CLe_1122") == 0) {
2178  CLe_1122 = value;
2179  } else if (name.compare("CLe_2211") == 0) {
2180  CLe_2211 = value;
2181  } else if (name.compare("CLe_1133") == 0) {
2182  CLe_1133 = value;
2183  } else if (name.compare("CLe_3311") == 0) {
2184  CLe_3311 = value;
2185  } else if (name.compare("CLu") == 0) {
2186  CLu_1111 = value;
2187  CLu_1122 = value;
2188  CLu_2211 = value;
2189  CLu_1133 = value;
2190  CLu_2233 = value;
2191  CLu_3311 = value;
2192  } else if (name.compare("CLu_1111") == 0) {
2193  CLu_1111 = value;
2194  } else if (name.compare("CLu_1122") == 0) {
2195  CLu_1122 = value;
2196  } else if (name.compare("CLu_2211") == 0) {
2197  CLu_2211 = value;
2198  } else if (name.compare("CLu_1133") == 0) {
2199  CLu_1133 = value;
2200  } else if (name.compare("CLu_2233") == 0) {
2201  CLu_2233 = value;
2202  } else if (name.compare("CLu_3311") == 0) {
2203  CLu_3311 = value;
2204  } else if (name.compare("CLd") == 0) {
2205  CLd_1111 = value;
2206  CLd_1122 = value;
2207  CLd_2211 = value;
2208  CLd_1133 = value;
2209  CLd_3311 = value;
2210  } else if (name.compare("CLd_1111") == 0) {
2211  CLd_1111 = value;
2212  } else if (name.compare("CLd_1122") == 0) {
2213  CLd_1122 = value;
2214  } else if (name.compare("CLd_2211") == 0) {
2215  CLd_2211 = value;
2216  } else if (name.compare("CLd_1133") == 0) {
2217  CLd_1133 = value;
2218  } else if (name.compare("CLd_3311") == 0) {
2219  CLd_3311 = value;
2220  } else if (name.compare("CLd_1123") == 0) {
2221  CLd_1123 = value;
2222  } else if (name.compare("CLd_2223") == 0) {
2223  CLd_2223 = value;
2224  } else if (name.compare("CLd_3323") == 0) {
2225  CLd_3323 = value;
2226  } else if (name.compare("CLd_1132") == 0) {
2227  CLd_1132 = value;
2228  } else if (name.compare("CLd_2232") == 0) {
2229  CLd_2232 = value;
2230  } else if (name.compare("CLd_3332") == 0) {
2231  CLd_3332 = value;
2232  } else if (name.compare("CQe") == 0) {
2233  CQe_1111 = value;
2234  CQe_1122 = value;
2235  CQe_2211 = value;
2236  CQe_1133 = value;
2237  CQe_3311 = value;
2238  } else if (name.compare("CQe_1111") == 0) {
2239  CQe_1111 = value;
2240  } else if (name.compare("CQe_1122") == 0) {
2241  CQe_1122 = value;
2242  } else if (name.compare("CQe_2211") == 0) {
2243  CQe_2211 = value;
2244  } else if (name.compare("CQe_1133") == 0) {
2245  CQe_1133 = value;
2246  } else if (name.compare("CQe_3311") == 0) {
2247  CQe_3311 = value;
2248  } else if (name.compare("CQe_2311") == 0) {
2249  CQe_2311 = value;
2250  } else if (name.compare("CQe_2322") == 0) {
2251  CQe_2322 = value;
2252  } else if (name.compare("CQe_2333") == 0) {
2253  CQe_2333 = value;
2254  } else if (name.compare("CQe_3211") == 0) {
2255  CQe_3211 = value;
2256  } else if (name.compare("CQe_3222") == 0) {
2257  CQe_3222 = value;
2258  } else if (name.compare("CLedQ_11") == 0) {
2259  CLedQ_11 = value;
2260  } else if (name.compare("CLedQ_22") == 0) {
2261  CLedQ_22 = value;
2262  } else if (name.compare("CpLedQ_11") == 0) {
2263  CpLedQ_11 = value;
2264  } else if (name.compare("CpLedQ_22") == 0) {
2265  CpLedQ_22 = value;
2266  } else if (name.compare("CQe_3233") == 0) {
2267  CQe_3233 = value;
2268  } else if (name.compare("Lambda_NP") == 0) {
2269  Lambda_NP = value;
2270  } else if (name.compare("BrHinv") == 0) {
2271 // Always positive
2272  BrHinv = fabs(value);
2273  } else if (name.compare("BrHexo") == 0) {
2274 // Always positive
2275  BrHexo = fabs(value);
2276  } else if (name.compare("dg1Z") == 0) {
2277  dg1Z = value;
2278  } else if (name.compare("dKappaga") == 0) {
2279  dKappaga = value;
2280  } else if (name.compare("lambZ") == 0) {
2281  lambZ = value;
2282  } else if (name.compare("eggFint") == 0) {
2283  eggFint = value;
2284  } else if (name.compare("eggFpar") == 0) {
2285  eggFpar = value;
2286  } else if (name.compare("ettHint") == 0) {
2287  ettHint = value;
2288  } else if (name.compare("ettHpar") == 0) {
2289  ettHpar = value;
2290  } else if (name.compare("eVBFint") == 0) {
2291  eVBFint = value;
2292  } else if (name.compare("eVBFpar") == 0) {
2293  eVBFpar = value;
2294  } else if (name.compare("eWHint") == 0) {
2295  eWHint = value;
2296  } else if (name.compare("eWHpar") == 0) {
2297  eWHpar = value;
2298  } else if (name.compare("eZHint") == 0) {
2299  eZHint = value;
2300  } else if (name.compare("eZHpar") == 0) {
2301  eZHpar = value;
2302  } else if (name.compare("eeeWBFint") == 0) {
2303  eeeWBFint = value;
2304  } else if (name.compare("eeeWBFpar") == 0) {
2305  eeeWBFpar = value;
2306  } else if (name.compare("eeeZHint") == 0) {
2307  eeeZHint = value;
2308  } else if (name.compare("eeeZHpar") == 0) {
2309  eeeZHpar = value;
2310  } else if (name.compare("eeettHint") == 0) {
2311  eeettHint = value;
2312  } else if (name.compare("eeettHpar") == 0) {
2313  eeettHpar = value;
2314  } else if (name.compare("eepWBFint") == 0) {
2315  eepWBFint = value;
2316  } else if (name.compare("eepWBFpar") == 0) {
2317  eepWBFpar = value;
2318  } else if (name.compare("eepZBFint") == 0) {
2319  eepZBFint = value;
2320  } else if (name.compare("eepZBFpar") == 0) {
2321  eepZBFpar = value;
2322  } else if (name.compare("eHggint") == 0) {
2323  eHggint = value;
2324  } else if (name.compare("eHggpar") == 0) {
2325  eHggpar = value;
2326  } else if (name.compare("eHWWint") == 0) {
2327  eHWWint = value;
2328  } else if (name.compare("eHWWpar") == 0) {
2329  eHWWpar = value;
2330  } else if (name.compare("eHZZint") == 0) {
2331  eHZZint = value;
2332  } else if (name.compare("eHZZpar") == 0) {
2333  eHZZpar = value;
2334  } else if (name.compare("eHZgaint") == 0) {
2335  eHZgaint = value;
2336  } else if (name.compare("eHZgapar") == 0) {
2337  eHZgapar = value;
2338  } else if (name.compare("eHgagaint") == 0) {
2339  eHgagaint = value;
2340  } else if (name.compare("eHgagapar") == 0) {
2341  eHgagapar = value;
2342  } else if (name.compare("eHmumuint") == 0) {
2343  eHmumuint = value;
2344  } else if (name.compare("eHmumupar") == 0) {
2345  eHmumupar = value;
2346  } else if (name.compare("eHtautauint") == 0) {
2347  eHtautauint = value;
2348  } else if (name.compare("eHtautaupar") == 0) {
2349  eHtautaupar = value;
2350  } else if (name.compare("eHccint") == 0) {
2351  eHccint = value;
2352  } else if (name.compare("eHccpar") == 0) {
2353  eHccpar = value;
2354  } else if (name.compare("eHbbint") == 0) {
2355  eHbbint = value;
2356  } else if (name.compare("eHbbpar") == 0) {
2357  eHbbpar = value;
2358  } else if (name.compare("eggFHgaga") == 0) {
2359  eggFHgaga = value;
2360  } else if (name.compare("eggFHZga") == 0) {
2361  eggFHZga = value;
2362  } else if (name.compare("eggFHZZ") == 0) {
2363  eggFHZZ = value;
2364  } else if (name.compare("eggFHWW") == 0) {
2365  eggFHWW = value;
2366  } else if (name.compare("eggFHtautau") == 0) {
2367  eggFHtautau = value;
2368  } else if (name.compare("eggFHbb") == 0) {
2369  eggFHbb = value;
2370  } else if (name.compare("eggFHmumu") == 0) {
2371  eggFHmumu = value;
2372  } else if (name.compare("eVBFHgaga") == 0) {
2373  eVBFHgaga = value;
2374  } else if (name.compare("eVBFHZga") == 0) {
2375  eVBFHZga = value;
2376  } else if (name.compare("eVBFHZZ") == 0) {
2377  eVBFHZZ = value;
2378  } else if (name.compare("eVBFHWW") == 0) {
2379  eVBFHWW = value;
2380  } else if (name.compare("eVBFHtautau") == 0) {
2381  eVBFHtautau = value;
2382  } else if (name.compare("eVBFHbb") == 0) {
2383  eVBFHbb = value;
2384  } else if (name.compare("eVBFHmumu") == 0) {
2385  eVBFHmumu = value;
2386  } else if (name.compare("eWHgaga") == 0) {
2387  eWHgaga = value;
2388  } else if (name.compare("eWHZga") == 0) {
2389  eWHZga = value;
2390  } else if (name.compare("eWHZZ") == 0) {
2391  eWHZZ = value;
2392  } else if (name.compare("eWHWW") == 0) {
2393  eWHWW = value;
2394  } else if (name.compare("eWHtautau") == 0) {
2395  eWHtautau = value;
2396  } else if (name.compare("eWHbb") == 0) {
2397  eWHbb = value;
2398  } else if (name.compare("eWHmumu") == 0) {
2399  eWHmumu = value;
2400  } else if (name.compare("eZHgaga") == 0) {
2401  eZHgaga = value;
2402  } else if (name.compare("eZHZga") == 0) {
2403  eZHZga = value;
2404  } else if (name.compare("eZHZZ") == 0) {
2405  eZHZZ = value;
2406  } else if (name.compare("eZHWW") == 0) {
2407  eZHWW = value;
2408  } else if (name.compare("eZHtautau") == 0) {
2409  eZHtautau = value;
2410  } else if (name.compare("eZHbb") == 0) {
2411  eZHbb = value;
2412  } else if (name.compare("eZHmumu") == 0) {
2413  eZHmumu = value;
2414  } else if (name.compare("ettHgaga") == 0) {
2415  ettHgaga = value;
2416  } else if (name.compare("ettHZga") == 0) {
2417  ettHZga = value;
2418  } else if (name.compare("ettHZZ") == 0) {
2419  ettHZZ = value;
2420  } else if (name.compare("ettHWW") == 0) {
2421  ettHWW = value;
2422  } else if (name.compare("ettHtautau") == 0) {
2423  ettHtautau = value;
2424  } else if (name.compare("ettHbb") == 0) {
2425  ettHbb = value;
2426  } else if (name.compare("ettHmumu") == 0) {
2427  ettHmumu = value;
2428  } else if (name.compare("eVBFHinv") == 0) {
2429  eVBFHinv = value;
2430  } else if (name.compare("eVHinv") == 0) {
2431  eVHinv = value;
2432  } else if (name.compare("eVBF_2_Hbox") == 0) {
2433  eVBF_2_Hbox = value;
2434  } else if (name.compare("eVBF_2_HQ1_11") == 0) {
2435  eVBF_2_HQ1_11 = value;
2436  } else if (name.compare("eVBF_2_Hu_11") == 0) {
2437  eVBF_2_Hu_11 = value;
2438  } else if (name.compare("eVBF_2_Hd_11") == 0) {
2439  eVBF_2_Hd_11 = value;
2440  } else if (name.compare("eVBF_2_HQ3_11") == 0) {
2441  eVBF_2_HQ3_11 = value;
2442  } else if (name.compare("eVBF_2_HD") == 0) {
2443  eVBF_2_HD = value;
2444  } else if (name.compare("eVBF_2_HB") == 0) {
2445  eVBF_2_HB = value;
2446  } else if (name.compare("eVBF_2_HW") == 0) {
2447  eVBF_2_HW = value;
2448  } else if (name.compare("eVBF_2_HWB") == 0) {
2449  eVBF_2_HWB = value;
2450  } else if (name.compare("eVBF_2_HG") == 0) {
2451  eVBF_2_HG = value;
2452  } else if (name.compare("eVBF_2_DHB") == 0) {
2453  eVBF_2_DHB = value;
2454  } else if (name.compare("eVBF_2_DHW") == 0) {
2455  eVBF_2_DHW = value;
2456  } else if (name.compare("eVBF_2_DeltaGF") == 0) {
2457  eVBF_2_DeltaGF = value;
2458  } else if (name.compare("eVBF_78_Hbox") == 0) {
2459  eVBF_78_Hbox = value;
2460  } else if (name.compare("eVBF_78_HQ1_11") == 0) {
2461  eVBF_78_HQ1_11 = value;
2462  } else if (name.compare("eVBF_78_Hu_11") == 0) {
2463  eVBF_78_Hu_11 = value;
2464  } else if (name.compare("eVBF_78_Hd_11") == 0) {
2465  eVBF_78_Hd_11 = value;
2466  } else if (name.compare("eVBF_78_HQ3_11") == 0) {
2467  eVBF_78_HQ3_11 = value;
2468  } else if (name.compare("eVBF_78_HD") == 0) {
2469  eVBF_78_HD = value;
2470  } else if (name.compare("eVBF_78_HB") == 0) {
2471  eVBF_78_HB = value;
2472  } else if (name.compare("eVBF_78_HW") == 0) {
2473  eVBF_78_HW = value;
2474  } else if (name.compare("eVBF_78_HWB") == 0) {
2475  eVBF_78_HWB = value;
2476  } else if (name.compare("eVBF_78_HG") == 0) {
2477  eVBF_78_HG = value;
2478  } else if (name.compare("eVBF_78_DHB") == 0) {
2479  eVBF_78_DHB = value;
2480  } else if (name.compare("eVBF_78_DHW") == 0) {
2481  eVBF_78_DHW = value;
2482  } else if (name.compare("eVBF_78_DeltaGF") == 0) {
2483  eVBF_78_DeltaGF = value;
2484  } else if (name.compare("eVBF_1314_Hbox") == 0) {
2485  eVBF_1314_Hbox = value;
2486  } else if (name.compare("eVBF_1314_HQ1_11") == 0) {
2487  eVBF_1314_HQ1_11 = value;
2488  } else if (name.compare("eVBF_1314_Hu_11") == 0) {
2489  eVBF_1314_Hu_11 = value;
2490  } else if (name.compare("eVBF_1314_Hd_11") == 0) {
2491  eVBF_1314_Hd_11 = value;
2492  } else if (name.compare("eVBF_1314_HQ3_11") == 0) {
2493  eVBF_1314_HQ3_11 = value;
2494  } else if (name.compare("eVBF_1314_HD") == 0) {
2495  eVBF_1314_HD = value;
2496  } else if (name.compare("eVBF_1314_HB") == 0) {
2497  eVBF_1314_HB = value;
2498  } else if (name.compare("eVBF_1314_HW") == 0) {
2499  eVBF_1314_HW = value;
2500  } else if (name.compare("eVBF_1314_HWB") == 0) {
2501  eVBF_1314_HWB = value;
2502  } else if (name.compare("eVBF_1314_HG") == 0) {
2503  eVBF_1314_HG = value;
2504  } else if (name.compare("eVBF_1314_DHB") == 0) {
2505  eVBF_1314_DHB = value;
2506  } else if (name.compare("eVBF_1314_DHW") == 0) {
2507  eVBF_1314_DHW = value;
2508  } else if (name.compare("eVBF_1314_DeltaGF") == 0) {
2509  eVBF_1314_DeltaGF = value;
2510  } else if (name.compare("eWH_2_Hbox") == 0) {
2511  eWH_2_Hbox = value;
2512  } else if (name.compare("eWH_2_HQ3_11") == 0) {
2513  eWH_2_HQ3_11 = value;
2514  } else if (name.compare("eWH_2_HD") == 0) {
2515  eWH_2_HD = value;
2516  } else if (name.compare("eWH_2_HW") == 0) {
2517  eWH_2_HW = value;
2518  } else if (name.compare("eWH_2_HWB") == 0) {
2519  eWH_2_HWB = value;
2520  } else if (name.compare("eWH_2_DHW") == 0) {
2521  eWH_2_DHW = value;
2522  } else if (name.compare("eWH_2_DeltaGF") == 0) {
2523  eWH_2_DeltaGF = value;
2524  } else if (name.compare("eWH_78_Hbox") == 0) {
2525  eWH_78_Hbox = value;
2526  } else if (name.compare("eWH_78_HQ3_11") == 0) {
2527  eWH_78_HQ3_11 = value;
2528  } else if (name.compare("eWH_78_HD") == 0) {
2529  eWH_78_HD = value;
2530  } else if (name.compare("eWH_78_HW") == 0) {
2531  eWH_78_HW = value;
2532  } else if (name.compare("eWH_78_HWB") == 0) {
2533  eWH_78_HWB = value;
2534  } else if (name.compare("eWH_78_DHW") == 0) {
2535  eWH_78_DHW = value;
2536  } else if (name.compare("eWH_78_DeltaGF") == 0) {
2537  eWH_78_DeltaGF = value;
2538  } else if (name.compare("eWH_1314_Hbox") == 0) {
2539  eWH_1314_Hbox = value;
2540  } else if (name.compare("eWH_1314_HQ3_11") == 0) {
2541  eWH_1314_HQ3_11 = value;
2542  } else if (name.compare("eWH_1314_HD") == 0) {
2543  eWH_1314_HD = value;
2544  } else if (name.compare("eWH_1314_HW") == 0) {
2545  eWH_1314_HW = value;
2546  } else if (name.compare("eWH_1314_HWB") == 0) {
2547  eWH_1314_HWB = value;
2548  } else if (name.compare("eWH_1314_DHW") == 0) {
2549  eWH_1314_DHW = value;
2550  } else if (name.compare("eWH_1314_DeltaGF") == 0) {
2551  eWH_1314_DeltaGF = value;
2552  } else if (name.compare("eZH_2_Hbox") == 0) {
2553  eZH_2_Hbox = value;
2554  } else if (name.compare("eZH_2_HQ1_11") == 0) {
2555  eZH_2_HQ1_11 = value;
2556  } else if (name.compare("eZH_2_Hu_11") == 0) {
2557  eZH_2_Hu_11 = value;
2558  } else if (name.compare("eZH_2_Hd_11") == 0) {
2559  eZH_2_Hd_11 = value;
2560  } else if (name.compare("eZH_2_HQ3_11") == 0) {
2561  eZH_2_HQ3_11 = value;
2562  } else if (name.compare("eZH_2_HD") == 0) {
2563  eZH_2_HD = value;
2564  } else if (name.compare("eZH_2_HB") == 0) {
2565  eZH_2_HB = value;
2566  } else if (name.compare("eZH_2_HW") == 0) {
2567  eZH_2_HW = value;
2568  } else if (name.compare("eZH_2_HWB") == 0) {
2569  eZH_2_HWB = value;
2570  } else if (name.compare("eZH_2_DHB") == 0) {
2571  eZH_2_DHB = value;
2572  } else if (name.compare("eZH_2_DHW") == 0) {
2573  eZH_2_DHW = value;
2574  } else if (name.compare("eZH_2_DeltaGF") == 0) {
2575  eZH_2_DeltaGF = value;
2576  } else if (name.compare("eZH_78_Hbox") == 0) {
2577  eZH_78_Hbox = value;
2578  } else if (name.compare("eZH_78_HQ1_11") == 0) {
2579  eZH_78_HQ1_11 = value;
2580  } else if (name.compare("eZH_78_Hu_11") == 0) {
2581  eZH_78_Hu_11 = value;
2582  } else if (name.compare("eZH_78_Hd_11") == 0) {
2583  eZH_78_Hd_11 = value;
2584  } else if (name.compare("eZH_78_HQ3_11") == 0) {
2585  eZH_78_HQ3_11 = value;
2586  } else if (name.compare("eZH_78_HD") == 0) {
2587  eZH_78_HD = value;
2588  } else if (name.compare("eZH_78_HB") == 0) {
2589  eZH_78_HB = value;
2590  } else if (name.compare("eZH_78_HW") == 0) {
2591  eZH_78_HW = value;
2592  } else if (name.compare("eZH_78_HWB") == 0) {
2593  eZH_78_HWB = value;
2594  } else if (name.compare("eZH_78_DHB") == 0) {
2595  eZH_78_DHB = value;
2596  } else if (name.compare("eZH_78_DHW") == 0) {
2597  eZH_78_DHW = value;
2598  } else if (name.compare("eZH_78_DeltaGF") == 0) {
2599  eZH_78_DeltaGF = value;
2600  } else if (name.compare("eZH_1314_Hbox") == 0) {
2601  eZH_1314_Hbox = value;
2602  } else if (name.compare("eZH_1314_HQ1_11") == 0) {
2603  eZH_1314_HQ1_11 = value;
2604  } else if (name.compare("eZH_1314_Hu_11") == 0) {
2605  eZH_1314_Hu_11 = value;
2606  } else if (name.compare("eZH_1314_Hd_11") == 0) {
2607  eZH_1314_Hd_11 = value;
2608  } else if (name.compare("eZH_1314_HQ3_11") == 0) {
2609  eZH_1314_HQ3_11 = value;
2610  } else if (name.compare("eZH_1314_HD") == 0) {
2611  eZH_1314_HD = value;
2612  } else if (name.compare("eZH_1314_HB") == 0) {
2613  eZH_1314_HB = value;
2614  } else if (name.compare("eZH_1314_HW") == 0) {
2615  eZH_1314_HW = value;
2616  } else if (name.compare("eZH_1314_HWB") == 0) {
2617  eZH_1314_HWB = value;
2618  } else if (name.compare("eZH_1314_DHB") == 0) {
2619  eZH_1314_DHB = value;
2620  } else if (name.compare("eZH_1314_DHW") == 0) {
2621  eZH_1314_DHW = value;
2622  } else if (name.compare("eZH_1314_DeltaGF") == 0) {
2623  eZH_1314_DeltaGF = value;
2624  } else if (name.compare("ettH_2_HG") == 0) {
2625  ettH_2_HG = value;
2626  } else if (name.compare("ettH_2_G") == 0) {
2627  ettH_2_G = value;
2628  } else if (name.compare("ettH_2_uG_33r") == 0) {
2629  ettH_2_uG_33r = value;
2630  } else if (name.compare("ettH_2_DeltagHt") == 0) {
2631  ettH_2_DeltagHt = value;
2632  } else if (name.compare("ettH_78_HG") == 0) {
2633  ettH_78_HG = value;
2634  } else if (name.compare("ettH_78_G") == 0) {
2635  ettH_78_G = value;
2636  } else if (name.compare("ettH_78_uG_33r") == 0) {
2637  ettH_78_uG_33r = value;
2638  } else if (name.compare("ettH_78_DeltagHt") == 0) {
2639  ettH_78_DeltagHt = value;
2640  } else if (name.compare("ettH_1314_HG") == 0) {
2641  ettH_1314_HG = value;
2642  } else if (name.compare("ettH_1314_G") == 0) {
2643  ettH_1314_G = value;
2644  } else if (name.compare("ettH_1314_uG_33r") == 0) {
2645  ettH_1314_uG_33r = value;
2646  } else if (name.compare("ettH_1314_DeltagHt") == 0) {
2647  ettH_1314_DeltagHt = value;
2648  } else
2649  NPbase::setParameter(name, value);
2650 }

◆ STXS_ggH0j()

double NPSMEFTd6::STXS_ggH0j ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15058 of file NPSMEFTd6.cpp.

15058  {
15059 
15060  double STXSb = 1.0;
15061 
15062  STXSb = 1.0 + 55.2*aiG + 0.362*ai3G + 0.276*ai2G;
15063 
15064  return STXSb;
15065 }

◆ STXS_ggH1j_pTH_0_60()

double NPSMEFTd6::STXS_ggH1j_pTH_0_60 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15068 of file NPSMEFTd6.cpp.

15068  {
15069 
15070  double STXSb = 1.0;
15071 
15072  STXSb = 1.0 + 56.0*aiG + 1.52*ai3G + 1.19*ai2G;
15073 
15074  return STXSb;
15075 }

◆ STXS_ggH1j_pTH_120_200()

double NPSMEFTd6::STXS_ggH1j_pTH_120_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15088 of file NPSMEFTd6.cpp.

15088  {
15089 
15090  double STXSb = 1.0;
15091 
15092  STXSb = 1.0 + 56.5*aiG + 17.8*ai3G + 11.2*ai2G;
15093 
15094  return STXSb;
15095 }

◆ STXS_ggH1j_pTH_200()

double NPSMEFTd6::STXS_ggH1j_pTH_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15098 of file NPSMEFTd6.cpp.

15098  {
15099 
15100  double STXSb = 1.0;
15101 
15102  STXSb = 1.0 + 55.0*aiG + 52.0*ai3G + 34.0*ai2G;
15103 
15104  return STXSb;
15105 }

◆ STXS_ggH1j_pTH_60_120()

double NPSMEFTd6::STXS_ggH1j_pTH_60_120 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15078 of file NPSMEFTd6.cpp.

15078  {
15079 
15080  double STXSb = 1.0;
15081 
15082  STXSb = 1.0 + 55.5*aiG + 4.12*ai3G + 2.76*ai2G;
15083 
15084  return STXSb;
15085 }

◆ STXS_ggH2j_pTH_0_200()

double NPSMEFTd6::STXS_ggH2j_pTH_0_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15108 of file NPSMEFTd6.cpp.

15108  {
15109 
15110  double STXSb = 1.0;
15111 
15112  return STXSb;
15113 }

◆ STXS_ggH2j_pTH_0_60()

double NPSMEFTd6::STXS_ggH2j_pTH_0_60 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15116 of file NPSMEFTd6.cpp.

15116  {
15117 
15118  double STXSb = 1.0;
15119 
15120  STXSb = 1.0 + 55.6*aiG + 3.66*ai3G + 4.23*ai2G;
15121 
15122  return STXSb;
15123 }

◆ STXS_ggH2j_pTH_120_200()

double NPSMEFTd6::STXS_ggH2j_pTH_120_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15134 of file NPSMEFTd6.cpp.

15134  {
15135 
15136  double STXSb = 1.0;
15137 
15138  STXSb = 1.0 + 55.8*aiG + 23.0*ai3G + 17.5*ai2G;
15139 
15140  return STXSb;
15141 }

◆ STXS_ggH2j_pTH_200()

double NPSMEFTd6::STXS_ggH2j_pTH_200 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15143 of file NPSMEFTd6.cpp.

15143  {
15144 
15145  double STXSb = 1.0;
15146 
15147  STXSb = 1.0 + 56.0*aiG + 89.8*ai3G + 68.1*ai2G;
15148 
15149  return STXSb;
15150 }

◆ STXS_ggH2j_pTH_60_120()

double NPSMEFTd6::STXS_ggH2j_pTH_60_120 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15125 of file NPSMEFTd6.cpp.

15125  {
15126 
15127  double STXSb = 1.0;
15128 
15129  STXSb = 1.0 + 56.1*aiG + 7.73*ai3G + 6.81*ai2G;
15130 
15131  return STXSb;
15132 }

◆ STXS_ggH_VBFtopo_j3()

double NPSMEFTd6::STXS_ggH_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15048 of file NPSMEFTd6.cpp.

15048  {
15049 
15050  double STXSb = 1.0;
15051 
15052  STXSb = 1.0 + 55.9*aiG + 9.04*ai3G + 8.1*ai2G;
15053 
15054  return STXSb;
15055 }

◆ STXS_ggH_VBFtopo_j3v()

double NPSMEFTd6::STXS_ggH_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \(gg \to H\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15039 of file NPSMEFTd6.cpp.

15039  {
15040 
15041  double STXSb = 1.0;
15042 
15043  STXSb = 1.0 + 56.6*aiG + 5.5*ai3G + 4.36*ai2G;
15044 
15045  return STXSb;
15046 }

◆ STXS_qqHll_pTV_0_150()

double NPSMEFTd6::STXS_qqHll_pTV_0_150 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15256 of file NPSMEFTd6.cpp.

15256  {
15257 
15258  double STXSb = 1.0;
15259 
15260  STXSb = 1.0 - 1.0*aiH - 4.001*aiT + 29.82*aiWW + 8.43*aiB + 8.5*aiHW
15261  + 2.545*aiHB + 0.0315*aiA - 1.89*aiHQ + 22.84*aipHQ + 5.247*aiHu
15262  - 2.0*aiHd - 0.963*aiHL + 2.042*aipHL - 0.2307*aiHe;
15263 
15264  return STXSb;
15265 }

◆ STXS_qqHll_pTV_150_250()

double NPSMEFTd6::STXS_qqHll_pTV_150_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15268 of file NPSMEFTd6.cpp.

15268  {
15269 
15270  double STXSb = 1.0;
15271 
15272  return STXSb;
15273 }

◆ STXS_qqHll_pTV_150_250_0j()

double NPSMEFTd6::STXS_qqHll_pTV_150_250_0j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15276 of file NPSMEFTd6.cpp.

15276  {
15277 
15278  double STXSb = 1.0;
15279 
15280  STXSb = 1.0 - 0.993*aiH - 4.0*aiT + 62.4*aiWW + 18.08*aiB + 37.6*aiHW
15281  + 11.22*aiHB - 5.03*aiHQ + 61.0*aipHQ + 14.39*aiHu - 5.17*aiHd
15282  - 0.977*aiHL + 2.08*aipHL - 0.234*aiHe;
15283 
15284  return STXSb;
15285 }

◆ STXS_qqHll_pTV_150_250_1j()

double NPSMEFTd6::STXS_qqHll_pTV_150_250_1j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15288 of file NPSMEFTd6.cpp.

15288  {
15289 
15290  double STXSb = 1.0;
15291 
15292  STXSb = 1.0 - 1.002*aiH - 4.01*aiT + 57.9*aiWW + 16.78*aiB + 32.8*aiHW
15293  + 9.86*aiHB - 4.58*aiHQ + 55.6*aipHQ + 13.54*aiHu - 4.56*aiHd
15294  - 0.989*aiHL + 2.09*aipHL - 0.235*aiHe;
15295 
15296  return STXSb;
15297 }

◆ STXS_qqHll_pTV_250()

double NPSMEFTd6::STXS_qqHll_pTV_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \ell\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15300 of file NPSMEFTd6.cpp.

15300  {
15301 
15302  double STXSb = 1.0;
15303 
15304  STXSb = 1.0 - 0.998*aiH - 4.0*aiT + 153.1*aiWW + 45.6*aiB + 126.4*aiHW
15305  + 37.9*aiHB - 13.85*aiHQ + 168.6*aipHQ + 41.7*aiHu - 13.48*aiHd
15306  - 0.977*aiHL + 2.09*aipHL - 0.238*aiHe;
15307 
15308  return STXSb;
15309 }

◆ STXS_qqHlv_pTV_0_150()

double NPSMEFTd6::STXS_qqHlv_pTV_0_150 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15216 of file NPSMEFTd6.cpp.

15216  {
15217 
15218  double STXSb = 1.0;
15219 
15220  STXSb = 1.0 - 1.001*aiH + 33.63*aiWW + 11.49*aiHW + 23.62*aipHQ + 2.013*aipHL;
15221 
15222  return STXSb;
15223 }

◆ STXS_qqHlv_pTV_0_250()

double NPSMEFTd6::STXS_qqHlv_pTV_0_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15208 of file NPSMEFTd6.cpp.

15208  {
15209 
15210  double STXSb = 1.0;
15211 
15212  return STXSb;
15213 }

◆ STXS_qqHlv_pTV_150_250_0j()

double NPSMEFTd6::STXS_qqHlv_pTV_150_250_0j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15226 of file NPSMEFTd6.cpp.

15226  {
15227 
15228  double STXSb = 1.0;
15229 
15230  STXSb = 1.0 - 0.998*aiH + 76.3*aiWW + 50.7*aiHW + 66.5*aipHQ + 2.03*aipHL;
15231 
15232  return STXSb;
15233 }

◆ STXS_qqHlv_pTV_150_250_1j()

double NPSMEFTd6::STXS_qqHlv_pTV_150_250_1j ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15236 of file NPSMEFTd6.cpp.

15236  {
15237 
15238  double STXSb = 1.0;
15239 
15240  STXSb = 1.0 - 1.006*aiH + 70.9*aiWW + 45.5*aiHW + 60.8*aipHQ + 2.04*aipHL;
15241 
15242  return STXSb;
15243 }

◆ STXS_qqHlv_pTV_250()

double NPSMEFTd6::STXS_qqHlv_pTV_250 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H \ell \nu\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15246 of file NPSMEFTd6.cpp.

15246  {
15247 
15248  double STXSb = 1.0;
15249 
15250  STXSb = 1.0 - 1.001*aiH + 196.5*aiWW + 169.4*aiHW + 186.3*aipHQ + 2.03*aipHL;
15251 
15252  return STXSb;
15253 }

◆ STXS_qqHqq_pTj_200()

double NPSMEFTd6::STXS_qqHqq_pTj_200 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15198 of file NPSMEFTd6.cpp.

15198  {
15199 
15200  double STXSb = 1.0;
15201 
15202  STXSb = 1.0 + 7.82*aiWW - 0.1868*aiB - 30.65*aiHW - 2.371*aiHB;
15203 
15204  return STXSb;
15205 }

◆ STXS_qqHqq_Rest()

double NPSMEFTd6::STXS_qqHqq_Rest ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15188 of file NPSMEFTd6.cpp.

15188  {
15189 
15190  double STXSb = 1.0;
15191 
15192  STXSb = 1.0 + 1.546*aiWW - 0.02509*aiB - 3.631*aiHW - 0.2361*aiHB;
15193 
15194  return STXSb;
15195 }

◆ STXS_qqHqq_VBFtopo_j3()

double NPSMEFTd6::STXS_qqHqq_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15168 of file NPSMEFTd6.cpp.

15168  {
15169 
15170  double STXSb = 1.0;
15171 
15172  STXSb = 1.0 + 1.204*aiWW - 0.02692*aiB - 5.76*aiHW - 0.4058*aiHB;
15173 
15174  return STXSb;
15175 }

◆ STXS_qqHqq_VBFtopo_j3v()

double NPSMEFTd6::STXS_qqHqq_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15159 of file NPSMEFTd6.cpp.

15159  {
15160 
15161  double STXSb = 1.0;
15162 
15163  STXSb = 1.0 + 1.256*aiWW - 0.02319*aiB - 4.31*aiHW - 0.2907*aiHB;
15164 
15165  return STXSb;
15166 }

◆ STXS_qqHqq_VBFtopo_Rest()

double NPSMEFTd6::STXS_qqHqq_VBFtopo_Rest ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15153 of file NPSMEFTd6.cpp.

15153  {
15154 
15155  return STXS_qqHqq_Rest(sqrt_s);
15156 }

◆ STXS_qqHqq_VHtopo()

double NPSMEFTd6::STXS_qqHqq_VHtopo ( const double  sqrt_s) const
virtual

The STXS bin \(qq \to H qq\).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15178 of file NPSMEFTd6.cpp.

15178  {
15179 
15180  double STXSb = 1.0;
15181 
15182  STXSb = 1.0 + 1.389*aiWW - 0.0284*aiB - 6.23*aiHW - 0.417*aiHB;
15183 
15184  return STXSb;
15185 }

◆ STXS_ttHtH()

double NPSMEFTd6::STXS_ttHtH ( const double  sqrt_s) const
virtual

The STXS bin \( ttH + tH \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15312 of file NPSMEFTd6.cpp.

15312  {
15313 
15314  double STXSb = 1.0;
15315 
15316  STXSb = 1.0 - 0.983*aiH + 2.949*aiu + 0.928*aiG + 313.6*aiuG
15317  + 27.48*ai3G - 13.09*ai2G;
15318 
15319  return STXSb;
15320 }

◆ STXS_WHqqHqq_pTj1_200()

double NPSMEFTd6::STXS_WHqqHqq_pTj1_200 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15358 of file NPSMEFTd6.cpp.

15358  {
15359 
15360  double STXSb = 1.0;
15361 
15362  STXSb = 1.0 - 1.003*aiH + 181.2*aiWW + 152.3*aiHW + 173.7*aipHQ;
15363 
15364  return STXSb;
15365 }

◆ STXS_WHqqHqq_Rest()

double NPSMEFTd6::STXS_WHqqHqq_Rest ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15349 of file NPSMEFTd6.cpp.

15349  {
15350 
15351  double STXSb = 1.0;
15352 
15353  STXSb = 1.0 - 1.002*aiH + 34.29*aiWW + 11.56*aiHW + 26.27*aipHQ;
15354 
15355  return STXSb;
15356 }

◆ STXS_WHqqHqq_VBFtopo_j3()

double NPSMEFTd6::STXS_WHqqHqq_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15331 of file NPSMEFTd6.cpp.

15331  {
15332 
15333  double STXSb = 1.0;
15334 
15335  STXSb = 1.0 - 1.04*aiH + 44.9*aiWW + 20.3*aiHW + 36.8*aipHQ;
15336 
15337  return STXSb;
15338 }

◆ STXS_WHqqHqq_VBFtopo_j3v()

double NPSMEFTd6::STXS_WHqqHqq_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15322 of file NPSMEFTd6.cpp.

15322  {
15323 
15324  double STXSb = 1.0;
15325 
15326  STXSb = 1.0 - 0.94*aiH + 39.5*aiWW + 13.8*aiHW + 32.1*aipHQ;
15327 
15328  return STXSb;
15329 }

◆ STXS_WHqqHqq_VH2j()

double NPSMEFTd6::STXS_WHqqHqq_VH2j ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to WH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15340 of file NPSMEFTd6.cpp.

15340  {
15341 
15342  double STXSb = 1.0;
15343 
15344  STXSb = 1.0 - 0.996*aiH + 45.57*aiWW + 23.66*aiHW + 37.55*aipHQ;
15345 
15346  return STXSb;
15347 }

◆ STXS_ZHqqHqq_pTj1_200()

double NPSMEFTd6::STXS_ZHqqHqq_pTj1_200 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15407 of file NPSMEFTd6.cpp.

15407  {
15408 
15409  double STXSb = 1.0;
15410 
15411  STXSb = 1.0 - 1.003*aiH - 4.03*aiT + 141.5*aiWW + 41.6*aiB + 112.5*aiHW
15412  + 33.6*aiHB - 11.52*aiHQ + 156.2*aipHQ + 38.9*aiHu - 12.53*aiHd;
15413 
15414  return STXSb;
15415 }

◆ STXS_ZHqqHqq_Rest()

double NPSMEFTd6::STXS_ZHqqHqq_Rest ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15397 of file NPSMEFTd6.cpp.

15397  {
15398 
15399  double STXSb = 1.0;
15400 
15401  STXSb = 1.0 - 1.001*aiH - 3.998*aiT + 30.89*aiWW + 8.35*aiB + 8.71*aiHW
15402  + 2.616*aiHB - 1.782*aiHQ + 26.1*aipHQ + 5.942*aiHu - 2.305*aiHd;
15403 
15404  return STXSb;
15405 }

◆ STXS_ZHqqHqq_VBFtopo_j3()

double NPSMEFTd6::STXS_ZHqqHqq_VBFtopo_j3 ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15377 of file NPSMEFTd6.cpp.

15377  {
15378 
15379  double STXSb = 1.0;
15380 
15381  STXSb = 1.0 - 0.97*aiH - 3.98*aiT + 38.1*aiWW + 10.5*aiB + 14.2*aiHW
15382  + 4.15*aiHB - 2.36*aiHQ + 34.5*aipHQ + 8.4*aiHu - 2.79*aiHd;
15383 
15384  return STXSb;
15385 }

◆ STXS_ZHqqHqq_VBFtopo_j3v()

double NPSMEFTd6::STXS_ZHqqHqq_VBFtopo_j3v ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15367 of file NPSMEFTd6.cpp.

15367  {
15368 
15369  double STXSb = 1.0;
15370 
15371  STXSb = 1.0 - 0.94*aiH - 4.0*aiT + 34.8*aiWW + 10.0*aiB + 9.9*aiHW
15372  + 3.04*aiHB - 2.14*aiHQ + 31.1*aipHQ + 7.6*aiHu - 2.59*aiHd;
15373 
15374  return STXSb;
15375 }

◆ STXS_ZHqqHqq_VH2j()

double NPSMEFTd6::STXS_ZHqqHqq_VH2j ( const double  sqrt_s) const
virtual

The STXS bin \( qq \to ZH \to H qq \).

Parameters
[in]sqrt_sthe center-of-mass energy in TeV

Reimplemented from NPbase.

Definition at line 15387 of file NPSMEFTd6.cpp.

15387  {
15388 
15389  double STXSb = 1.0;
15390 
15391  STXSb = 1.0 - 0.998*aiH - 4.002*aiT + 37.99*aiWW + 10.47*aiB + 16.45*aiHW
15392  + 4.927*aiHB - 2.401*aiHQ + 34.45*aipHQ + 7.94*aiHu - 2.993*aiHd;
15393 
15394  return STXSb;
15395 }

◆ xseeWW()

double NPSMEFTd6::xseeWW ( const double  sqrt_s) const
virtual

Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).

Returns
\(\sigma(e^+ e^- \to W^+ W^- \to jj \ell \nu) \)

Reimplemented from NPbase.

Definition at line 14233 of file NPSMEFTd6.cpp.

14234 {
14235  return dxseeWWdcosBin(sqrt_s, -1.0, 1.0);
14236 }

Member Data Documentation

◆ ai2G

double NPSMEFTd6::ai2G
protected

Definition at line 5035 of file NPSMEFTd6.h.

◆ ai3G

double NPSMEFTd6::ai3G
protected

Definition at line 5035 of file NPSMEFTd6.h.

◆ aiA

double NPSMEFTd6::aiA
protected

Definition at line 5037 of file NPSMEFTd6.h.

◆ aiB

double NPSMEFTd6::aiB
protected

Definition at line 5036 of file NPSMEFTd6.h.

◆ aiG

double NPSMEFTd6::aiG
protected

Definition at line 5035 of file NPSMEFTd6.h.

◆ aiH

double NPSMEFTd6::aiH
protected

Definition at line 5036 of file NPSMEFTd6.h.

◆ aiHB

double NPSMEFTd6::aiHB
protected

Definition at line 5036 of file NPSMEFTd6.h.

◆ aiHd

double NPSMEFTd6::aiHd
protected

Definition at line 5038 of file NPSMEFTd6.h.

◆ aiHe

double NPSMEFTd6::aiHe
protected

Definition at line 5038 of file NPSMEFTd6.h.

◆ aiHL

double NPSMEFTd6::aiHL
protected

Definition at line 5038 of file NPSMEFTd6.h.

◆ aiHQ

double NPSMEFTd6::aiHQ
protected

Definition at line 5038 of file NPSMEFTd6.h.

◆ aiHu

double NPSMEFTd6::aiHu
protected

Definition at line 5038 of file NPSMEFTd6.h.

◆ aiHW

double NPSMEFTd6::aiHW
protected

Definition at line 5036 of file NPSMEFTd6.h.

◆ aipHL

double NPSMEFTd6::aipHL
protected

Definition at line 5038 of file NPSMEFTd6.h.

◆ aipHQ

double NPSMEFTd6::aipHQ
protected

Definition at line 5038 of file NPSMEFTd6.h.

◆ aiT

double NPSMEFTd6::aiT
protected

Definition at line 5036 of file NPSMEFTd6.h.

◆ aiu

double NPSMEFTd6::aiu
protected

Definition at line 5039 of file NPSMEFTd6.h.

◆ aiuG

double NPSMEFTd6::aiuG
protected

Definition at line 5039 of file NPSMEFTd6.h.

◆ aiWW

double NPSMEFTd6::aiWW
protected

Definition at line 5036 of file NPSMEFTd6.h.

◆ aleMz

double NPSMEFTd6::aleMz
protected

The em constant at Mz.

Definition at line 4995 of file NPSMEFTd6.h.

◆ BrHexo

double NPSMEFTd6::BrHexo
protected

The branching ratio of exotic (not invisible) Higgs decays.

Definition at line 4915 of file NPSMEFTd6.h.

◆ BrHinv

double NPSMEFTd6::BrHinv
protected

The branching ratio of invisible Higgs decays.

Definition at line 4914 of file NPSMEFTd6.h.

◆ C2B

double NPSMEFTd6::C2B
protected

The dimension-6 operator coefficient \(C_{2W}\).

Definition at line 4475 of file NPSMEFTd6.h.

◆ C2BS

double NPSMEFTd6::C2BS
protected

The dimension-6 operator coefficient \(C_{2W}^{SILH}\).

Definition at line 4477 of file NPSMEFTd6.h.

◆ C2W

double NPSMEFTd6::C2W
protected

The dimension-6 operator coefficient \(C_{2B}\).

Definition at line 4476 of file NPSMEFTd6.h.

◆ C2WS

double NPSMEFTd6::C2WS
protected

The dimension-6 operator coefficient \(C_{2B}^{SILH}\).

Definition at line 4478 of file NPSMEFTd6.h.

◆ CDB

double NPSMEFTd6::CDB
protected

The dimension-6 operator coefficient \(C_{DB}\).

Definition at line 4486 of file NPSMEFTd6.h.

◆ CdB_11i

double NPSMEFTd6::CdB_11i
protected

The dimension-6 operator coefficient \((C_{dB})_{11}\) (imaginary part).

Definition at line 4670 of file NPSMEFTd6.h.

◆ CdB_11r

double NPSMEFTd6::CdB_11r
protected

The dimension-6 operator coefficient \((C_{dB})_{11}\) (real part).

Definition at line 4664 of file NPSMEFTd6.h.

◆ CdB_12i

double NPSMEFTd6::CdB_12i
protected

The dimension-6 operator coefficient \((C_{dB})_{12}\) (imaginary part).

Definition at line 4671 of file NPSMEFTd6.h.

◆ CdB_12r

double NPSMEFTd6::CdB_12r
protected

The dimension-6 operator coefficient \((C_{dB})_{12}\) (real part).

Definition at line 4665 of file NPSMEFTd6.h.

◆ CdB_13i

double NPSMEFTd6::CdB_13i
protected

The dimension-6 operator coefficient \((C_{dB})_{13}\) (imaginary part).

Definition at line 4672 of file NPSMEFTd6.h.

◆ CdB_13r

double NPSMEFTd6::CdB_13r
protected

The dimension-6 operator coefficient \((C_{dB})_{13}\) (real part).

Definition at line 4666 of file NPSMEFTd6.h.

◆ CdB_22i

double NPSMEFTd6::CdB_22i
protected

The dimension-6 operator coefficient \((C_{dB})_{22}\) (imaginary part).

Definition at line 4673 of file NPSMEFTd6.h.

◆ CdB_22r

double NPSMEFTd6::CdB_22r
protected

The dimension-6 operator coefficient \((C_{dB})_{22}\) (real part).

Definition at line 4667 of file NPSMEFTd6.h.

◆ CdB_23i

double NPSMEFTd6::CdB_23i
protected

The dimension-6 operator coefficient \((C_{dB})_{23}\) (imaginary part).

Definition at line 4674 of file NPSMEFTd6.h.

◆ CdB_23r

double NPSMEFTd6::CdB_23r
protected

The dimension-6 operator coefficient \((C_{dB})_{23}\) (real part).

Definition at line 4668 of file NPSMEFTd6.h.

◆ CdB_33i

double NPSMEFTd6::CdB_33i
protected

The dimension-6 operator coefficient \((C_{dB})_{33}\) (imaginary part).

Definition at line 4675 of file NPSMEFTd6.h.

◆ CdB_33r

double NPSMEFTd6::CdB_33r
protected

The dimension-6 operator coefficient \((C_{dB})_{33}\) (real part).

Definition at line 4669 of file NPSMEFTd6.h.

◆ CdG_11i

double NPSMEFTd6::CdG_11i
protected

The dimension-6 operator coefficient \((C_{dG})_{11}\) (imaginary part).

Definition at line 4646 of file NPSMEFTd6.h.

◆ CdG_11r

double NPSMEFTd6::CdG_11r
protected

The dimension-6 operator coefficient \((C_{dG})_{11}\) (real part).

Definition at line 4640 of file NPSMEFTd6.h.

◆ CdG_12i

double NPSMEFTd6::CdG_12i
protected

The dimension-6 operator coefficient \((C_{dG})_{12}\) (imaginary part).

Definition at line 4647 of file NPSMEFTd6.h.

◆ CdG_12r

double NPSMEFTd6::CdG_12r
protected

The dimension-6 operator coefficient \((C_{dG})_{12}\) (real part).

Definition at line 4641 of file NPSMEFTd6.h.

◆ CdG_13i

double NPSMEFTd6::CdG_13i
protected

The dimension-6 operator coefficient \((C_{dG})_{13}\) (imaginary part).

Definition at line 4648 of file NPSMEFTd6.h.

◆ CdG_13r

double NPSMEFTd6::CdG_13r
protected

The dimension-6 operator coefficient \((C_{dG})_{13}\) (real part).

Definition at line 4642 of file NPSMEFTd6.h.

◆ CdG_22i

double NPSMEFTd6::CdG_22i
protected

The dimension-6 operator coefficient \((C_{dG})_{22}\) (imaginary part).

Definition at line 4649 of file NPSMEFTd6.h.

◆ CdG_22r

double NPSMEFTd6::CdG_22r
protected

The dimension-6 operator coefficient \((C_{dG})_{22}\) (real part).

Definition at line 4643 of file NPSMEFTd6.h.

◆ CdG_23i

double NPSMEFTd6::CdG_23i
protected

The dimension-6 operator coefficient \((C_{dG})_{23}\) (imaginary part).

Definition at line 4650 of file NPSMEFTd6.h.

◆ CdG_23r

double NPSMEFTd6::CdG_23r
protected

The dimension-6 operator coefficient \((C_{dG})_{23}\) (real part).

Definition at line 4644 of file NPSMEFTd6.h.

◆ CdG_33i

double NPSMEFTd6::CdG_33i
protected

The dimension-6 operator coefficient \((C_{dG})_{33}\) (imaginary part).

Definition at line 4651 of file NPSMEFTd6.h.

◆ CdG_33r

double NPSMEFTd6::CdG_33r
protected

The dimension-6 operator coefficient \((C_{dG})_{33}\) (real part).

Definition at line 4645 of file NPSMEFTd6.h.

◆ CdH_11i

double NPSMEFTd6::CdH_11i
protected

The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part).

Definition at line 4598 of file NPSMEFTd6.h.

◆ CdH_11r

double NPSMEFTd6::CdH_11r
protected

The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part).

Definition at line 4592 of file NPSMEFTd6.h.

◆ CdH_12i

double NPSMEFTd6::CdH_12i
protected

The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part).

Definition at line 4599 of file NPSMEFTd6.h.

◆ CdH_12r

double NPSMEFTd6::CdH_12r
protected

The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part).

Definition at line 4593 of file NPSMEFTd6.h.

◆ CdH_13i

double NPSMEFTd6::CdH_13i
protected

The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part).

Definition at line 4600 of file NPSMEFTd6.h.

◆ CdH_13r

double NPSMEFTd6::CdH_13r
protected

The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part).

Definition at line 4594 of file NPSMEFTd6.h.

◆ CdH_22i

double NPSMEFTd6::CdH_22i
protected

The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part).

Definition at line 4601 of file NPSMEFTd6.h.

◆ CdH_22r

double NPSMEFTd6::CdH_22r
protected

The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part).

Definition at line 4595 of file NPSMEFTd6.h.

◆ CdH_23i

double NPSMEFTd6::CdH_23i
protected

The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part).

Definition at line 4602 of file NPSMEFTd6.h.

◆ CdH_23r

double NPSMEFTd6::CdH_23r
protected

The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part).

Definition at line 4596 of file NPSMEFTd6.h.

◆ CdH_33i

double NPSMEFTd6::CdH_33i
protected

The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part).

Definition at line 4603 of file NPSMEFTd6.h.

◆ CdH_33r

double NPSMEFTd6::CdH_33r
protected

The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part).

Definition at line 4597 of file NPSMEFTd6.h.

◆ CDHB

double NPSMEFTd6::CDHB
protected

The dimension-6 operator coefficient \(C_{DHB}\).

Definition at line 4484 of file NPSMEFTd6.h.

◆ CDHW

double NPSMEFTd6::CDHW
protected

The dimension-6 operator coefficient \(C_{DHW}\).

Definition at line 4485 of file NPSMEFTd6.h.

◆ CDW

double NPSMEFTd6::CDW
protected

The dimension-6 operator coefficient \(C_{DW}\).

Definition at line 4487 of file NPSMEFTd6.h.

◆ CdW_11i

double NPSMEFTd6::CdW_11i
protected

The dimension-6 operator coefficient \((C_{dW})_{11}\) (imaginary part).

Definition at line 4658 of file NPSMEFTd6.h.

◆ CdW_11r

double NPSMEFTd6::CdW_11r
protected

The dimension-6 operator coefficient \((C_{dW})_{11}\) (real part).

Definition at line 4652 of file NPSMEFTd6.h.

◆ CdW_12i

double NPSMEFTd6::CdW_12i
protected

The dimension-6 operator coefficient \((C_{dW})_{12}\) (imaginary part).

Definition at line 4659 of file NPSMEFTd6.h.

◆ CdW_12r

double NPSMEFTd6::CdW_12r
protected

The dimension-6 operator coefficient \((C_{dW})_{12}\) (real part).

Definition at line 4653 of file NPSMEFTd6.h.

◆ CdW_13i

double NPSMEFTd6::CdW_13i
protected

The dimension-6 operator coefficient \((C_{dW})_{13}\) (imaginary part).

Definition at line 4660 of file NPSMEFTd6.h.

◆ CdW_13r

double NPSMEFTd6::CdW_13r
protected

The dimension-6 operator coefficient \((C_{dW})_{13}\) (real part).

Definition at line 4654 of file NPSMEFTd6.h.

◆ CdW_22i

double NPSMEFTd6::CdW_22i
protected

The dimension-6 operator coefficient \((C_{dW})_{22}\) (imaginary part).

Definition at line 4661 of file NPSMEFTd6.h.

◆ CdW_22r

double NPSMEFTd6::CdW_22r
protected

The dimension-6 operator coefficient \((C_{dW})_{22}\) (real part).

Definition at line 4655 of file NPSMEFTd6.h.

◆ CdW_23i

double NPSMEFTd6::CdW_23i
protected

The dimension-6 operator coefficient \((C_{dW})_{23}\) (imaginary part).

Definition at line 4662 of file NPSMEFTd6.h.

◆ CdW_23r

double NPSMEFTd6::CdW_23r
protected

The dimension-6 operator coefficient \((C_{dW})_{23}\) (real part).

Definition at line 4656 of file NPSMEFTd6.h.

◆ CdW_33i

double NPSMEFTd6::CdW_33i
protected

The dimension-6 operator coefficient \((C_{dW})_{33}\) (imaginary part).

Definition at line 4663 of file NPSMEFTd6.h.

◆ CdW_33r

double NPSMEFTd6::CdW_33r
protected

The dimension-6 operator coefficient \((C_{dW})_{33}\) (real part).

Definition at line 4657 of file NPSMEFTd6.h.

◆ CeB_11i

double NPSMEFTd6::CeB_11i
protected

The dimension-6 operator coefficient \((C_{eB})_{11}\) (imaginary part).

Definition at line 4694 of file NPSMEFTd6.h.

◆ CeB_11r

double NPSMEFTd6::CeB_11r
protected

The dimension-6 operator coefficient \((C_{eB})_{11}\) (real part).

Definition at line 4688 of file NPSMEFTd6.h.

◆ CeB_12i

double NPSMEFTd6::CeB_12i
protected

The dimension-6 operator coefficient \((C_{eB})_{12}\) (imaginary part).

Definition at line 4695 of file NPSMEFTd6.h.

◆ CeB_12r

double NPSMEFTd6::CeB_12r
protected

The dimension-6 operator coefficient \((C_{eB})_{12}\) (real part).

Definition at line 4689 of file NPSMEFTd6.h.

◆ CeB_13i

double NPSMEFTd6::CeB_13i
protected

The dimension-6 operator coefficient \((C_{eB})_{13}\) (imaginary part).

Definition at line 4696 of file NPSMEFTd6.h.

◆ CeB_13r

double NPSMEFTd6::CeB_13r
protected

The dimension-6 operator coefficient \((C_{eB})_{13}\) (real part).

Definition at line 4690 of file NPSMEFTd6.h.

◆ CeB_22i

double NPSMEFTd6::CeB_22i
protected

The dimension-6 operator coefficient \((C_{eB})_{22}\) (imaginary part).

Definition at line 4697 of file NPSMEFTd6.h.

◆ CeB_22r

double NPSMEFTd6::CeB_22r
protected

The dimension-6 operator coefficient \((C_{eB})_{22}\) (real part).

Definition at line 4691 of file NPSMEFTd6.h.

◆ CeB_23i

double NPSMEFTd6::CeB_23i
protected

The dimension-6 operator coefficient \((C_{eB})_{23}\) (imaginary part).

Definition at line 4698 of file NPSMEFTd6.h.

◆ CeB_23r

double NPSMEFTd6::CeB_23r
protected

The dimension-6 operator coefficient \((C_{eB})_{23}\) (real part).

Definition at line 4692 of file NPSMEFTd6.h.

◆ CeB_33i

double NPSMEFTd6::CeB_33i
protected

The dimension-6 operator coefficient \((C_{eB})_{33}\) (imaginary part).

Definition at line 4699 of file NPSMEFTd6.h.

◆ CeB_33r

double NPSMEFTd6::CeB_33r
protected

The dimension-6 operator coefficient \((C_{eB})_{33}\) (real part).

Definition at line 4693 of file NPSMEFTd6.h.

◆ Ced_1111

double NPSMEFTd6::Ced_1111
protected

Definition at line 4720 of file NPSMEFTd6.h.

◆ Ced_1122

double NPSMEFTd6::Ced_1122
protected

Definition at line 4721 of file NPSMEFTd6.h.

◆ Ced_1123

double NPSMEFTd6::Ced_1123
protected

Definition at line 4723 of file NPSMEFTd6.h.

◆ Ced_1132

double NPSMEFTd6::Ced_1132
protected

Definition at line 4724 of file NPSMEFTd6.h.

◆ Ced_1133

double NPSMEFTd6::Ced_1133
protected

Definition at line 4722 of file NPSMEFTd6.h.

◆ Ced_2211

double NPSMEFTd6::Ced_2211
protected

Definition at line 4721 of file NPSMEFTd6.h.

◆ Ced_2223

double NPSMEFTd6::Ced_2223
protected

Definition at line 4723 of file NPSMEFTd6.h.

◆ Ced_2232

double NPSMEFTd6::Ced_2232
protected

Definition at line 4724 of file NPSMEFTd6.h.

◆ Ced_3311

double NPSMEFTd6::Ced_3311
protected

Definition at line 4722 of file NPSMEFTd6.h.

◆ Ced_3323

double NPSMEFTd6::Ced_3323
protected

Definition at line 4723 of file NPSMEFTd6.h.

◆ Ced_3332

double NPSMEFTd6::Ced_3332
protected

Definition at line 4724 of file NPSMEFTd6.h.

◆ Cee_1111

double NPSMEFTd6::Cee_1111
protected

Definition at line 4713 of file NPSMEFTd6.h.

◆ Cee_1122

double NPSMEFTd6::Cee_1122
protected

Definition at line 4714 of file NPSMEFTd6.h.

◆ Cee_1133

double NPSMEFTd6::Cee_1133
protected

Definition at line 4715 of file NPSMEFTd6.h.

◆ Cee_2211

double NPSMEFTd6::Cee_2211
protected

Definition at line 4714 of file NPSMEFTd6.h.

◆ Cee_3311

double NPSMEFTd6::Cee_3311
protected

Definition at line 4715 of file NPSMEFTd6.h.

◆ CeH_11i

double NPSMEFTd6::CeH_11i
protected

The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part).

Definition at line 4574 of file NPSMEFTd6.h.

◆ CeH_11r

double NPSMEFTd6::CeH_11r
protected

The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part).

Definition at line 4568 of file NPSMEFTd6.h.

◆ CeH_12i

double NPSMEFTd6::CeH_12i
protected

The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part).

Definition at line 4575 of file NPSMEFTd6.h.

◆ CeH_12r

double NPSMEFTd6::CeH_12r
protected

The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part).

Definition at line 4569 of file NPSMEFTd6.h.

◆ CeH_13i

double NPSMEFTd6::CeH_13i
protected

The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part).

Definition at line 4576 of file NPSMEFTd6.h.

◆ CeH_13r

double NPSMEFTd6::CeH_13r
protected

The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part).

Definition at line 4570 of file NPSMEFTd6.h.

◆ CeH_22i

double NPSMEFTd6::CeH_22i
protected

The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part).

Definition at line 4577 of file NPSMEFTd6.h.

◆ CeH_22r

double NPSMEFTd6::CeH_22r
protected

The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part).

Definition at line 4571 of file NPSMEFTd6.h.

◆ CeH_23i

double NPSMEFTd6::CeH_23i
protected

The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part).

Definition at line 4578 of file NPSMEFTd6.h.

◆ CeH_23r

double NPSMEFTd6::CeH_23r
protected

The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part).

Definition at line 4572 of file NPSMEFTd6.h.

◆ CeH_33i

double NPSMEFTd6::CeH_33i
protected

The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part).

Definition at line 4579 of file NPSMEFTd6.h.

◆ CeH_33r

double NPSMEFTd6::CeH_33r
protected

The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part).

Definition at line 4573 of file NPSMEFTd6.h.

◆ Ceu_1111

double NPSMEFTd6::Ceu_1111
protected

Definition at line 4716 of file NPSMEFTd6.h.

◆ Ceu_1122

double NPSMEFTd6::Ceu_1122
protected

Definition at line 4717 of file NPSMEFTd6.h.

◆ Ceu_1133

double NPSMEFTd6::Ceu_1133
protected

Definition at line 4718 of file NPSMEFTd6.h.

◆ Ceu_2211

double NPSMEFTd6::Ceu_2211
protected

Definition at line 4717 of file NPSMEFTd6.h.

◆ Ceu_2233

double NPSMEFTd6::Ceu_2233
protected

Definition at line 4719 of file NPSMEFTd6.h.

◆ Ceu_3311

double NPSMEFTd6::Ceu_3311
protected

Definition at line 4718 of file NPSMEFTd6.h.

◆ CeW_11i

double NPSMEFTd6::CeW_11i
protected

The dimension-6 operator coefficient \((C_{eW})_{11}\) (imaginary part).

Definition at line 4682 of file NPSMEFTd6.h.

◆ CeW_11r

double NPSMEFTd6::CeW_11r
protected

The dimension-6 operator coefficient \((C_{eW})_{11}\) (real part).

Definition at line 4676 of file NPSMEFTd6.h.

◆ CeW_12i

double NPSMEFTd6::CeW_12i
protected

The dimension-6 operator coefficient \((C_{eW})_{12}\) (imaginary part).

Definition at line 4683 of file NPSMEFTd6.h.

◆ CeW_12r

double NPSMEFTd6::CeW_12r
protected

The dimension-6 operator coefficient \((C_{eW})_{12}\) (real part).

Definition at line 4677 of file NPSMEFTd6.h.

◆ CeW_13i

double NPSMEFTd6::CeW_13i
protected

The dimension-6 operator coefficient \((C_{eW})_{13}\) (imaginary part).

Definition at line 4684 of file NPSMEFTd6.h.

◆ CeW_13r

double NPSMEFTd6::CeW_13r
protected

The dimension-6 operator coefficient \((C_{eW})_{13}\) (real part).

Definition at line 4678 of file NPSMEFTd6.h.

◆ CeW_22i

double NPSMEFTd6::CeW_22i
protected

The dimension-6 operator coefficient \((C_{eW})_{22}\) (imaginary part).

Definition at line 4685 of file NPSMEFTd6.h.

◆ CeW_22r

double NPSMEFTd6::CeW_22r
protected

The dimension-6 operator coefficient \((C_{eW})_{22}\) (real part).

Definition at line 4679 of file NPSMEFTd6.h.

◆ CeW_23i

double NPSMEFTd6::CeW_23i
protected

The dimension-6 operator coefficient \((C_{eW})_{23}\) (imaginary part).

Definition at line 4686 of file NPSMEFTd6.h.

◆ CeW_23r

double NPSMEFTd6::CeW_23r
protected

The dimension-6 operator coefficient \((C_{eW})_{23}\) (real part).

Definition at line 4680 of file NPSMEFTd6.h.

◆ CeW_33i

double NPSMEFTd6::CeW_33i
protected

The dimension-6 operator coefficient \((C_{eW})_{33}\) (imaginary part).

Definition at line 4687 of file NPSMEFTd6.h.

◆ CeW_33r

double NPSMEFTd6::CeW_33r
protected

The dimension-6 operator coefficient \((C_{eW})_{33}\) (real part).

Definition at line 4681 of file NPSMEFTd6.h.

◆ CG

double NPSMEFTd6::CG
protected

The dimension-6 operator coefficient \(C_{G}\).

Definition at line 4473 of file NPSMEFTd6.h.

◆ CH

double NPSMEFTd6::CH
protected

The dimension-6 operator coefficient \(C_{H}\).

Definition at line 4492 of file NPSMEFTd6.h.

◆ CHB

double NPSMEFTd6::CHB
protected

The dimension-6 operator coefficient \(C_{HB}\).

Definition at line 4481 of file NPSMEFTd6.h.

◆ CHbox

double NPSMEFTd6::CHbox
protected

The dimension-6 operator coefficient \(C_{H\Box}\).

Definition at line 4491 of file NPSMEFTd6.h.

◆ CHD

double NPSMEFTd6::CHD
protected

The dimension-6 operator coefficient \(C_{HD}\).

Definition at line 4489 of file NPSMEFTd6.h.

◆ CHd_11

double NPSMEFTd6::CHd_11
protected

The dimension-6 operator coefficient \((C_{Hd})_{11}\).

Definition at line 4547 of file NPSMEFTd6.h.

◆ CHd_12i

double NPSMEFTd6::CHd_12i
protected

The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part).

Definition at line 4553 of file NPSMEFTd6.h.

◆ CHd_12r

double NPSMEFTd6::CHd_12r
protected

The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part).

Definition at line 4548 of file NPSMEFTd6.h.

◆ CHd_13i

double NPSMEFTd6::CHd_13i
protected

The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part).

Definition at line 4554 of file NPSMEFTd6.h.

◆ CHd_13r

double NPSMEFTd6::CHd_13r
protected

The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part).

Definition at line 4549 of file NPSMEFTd6.h.

◆ CHd_22

double NPSMEFTd6::CHd_22
protected

The dimension-6 operator coefficient \((C_{Hd})_{22}\).

Definition at line 4550 of file NPSMEFTd6.h.

◆ CHd_23i

double NPSMEFTd6::CHd_23i
protected

The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part).

Definition at line 4555 of file NPSMEFTd6.h.

◆ CHd_23r

double NPSMEFTd6::CHd_23r
protected

The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part).

Definition at line 4551 of file NPSMEFTd6.h.

◆ CHd_33

double NPSMEFTd6::CHd_33
protected

The dimension-6 operator coefficient \((C_{Hd})_{33}\).

Definition at line 4552 of file NPSMEFTd6.h.

◆ CHe_11

double NPSMEFTd6::CHe_11
protected

The dimension-6 operator coefficient \((C_{He})_{11}\).

Definition at line 4511 of file NPSMEFTd6.h.

◆ CHe_12i

double NPSMEFTd6::CHe_12i
protected

The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part).

Definition at line 4517 of file NPSMEFTd6.h.

◆ CHe_12r

double NPSMEFTd6::CHe_12r
protected

The dimension-6 operator coefficient \((C_{He})_{12}\) (real part).

Definition at line 4512 of file NPSMEFTd6.h.

◆ CHe_13i

double NPSMEFTd6::CHe_13i
protected

The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part).

Definition at line 4518 of file NPSMEFTd6.h.

◆ CHe_13r

double NPSMEFTd6::CHe_13r
protected

The dimension-6 operator coefficient \((C_{He})_{13}\) (real part).

Definition at line 4513 of file NPSMEFTd6.h.

◆ CHe_22

double NPSMEFTd6::CHe_22
protected

The dimension-6 operator coefficient \((C_{He})_{22}\).

Definition at line 4514 of file NPSMEFTd6.h.

◆ CHe_23i

double NPSMEFTd6::CHe_23i
protected

The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part).

Definition at line 4519 of file NPSMEFTd6.h.

◆ CHe_23r

double NPSMEFTd6::CHe_23r
protected

The dimension-6 operator coefficient \((C_{He})_{23}\) (real part).

Definition at line 4515 of file NPSMEFTd6.h.

◆ CHe_33

double NPSMEFTd6::CHe_33
protected

The dimension-6 operator coefficient \((C_{He})_{33}\).

Definition at line 4516 of file NPSMEFTd6.h.

◆ CHG

double NPSMEFTd6::CHG
protected

The dimension-6 operator coefficient \(C_{HG}\).

Definition at line 4479 of file NPSMEFTd6.h.

◆ CHL1_11

double NPSMEFTd6::CHL1_11
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).

Definition at line 4493 of file NPSMEFTd6.h.

◆ CHL1_12i

double NPSMEFTd6::CHL1_12i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).

Definition at line 4499 of file NPSMEFTd6.h.

◆ CHL1_12r

double NPSMEFTd6::CHL1_12r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).

Definition at line 4494 of file NPSMEFTd6.h.

◆ CHL1_13i

double NPSMEFTd6::CHL1_13i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).

Definition at line 4500 of file NPSMEFTd6.h.

◆ CHL1_13r

double NPSMEFTd6::CHL1_13r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).

Definition at line 4495 of file NPSMEFTd6.h.

◆ CHL1_22

double NPSMEFTd6::CHL1_22
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).

Definition at line 4496 of file NPSMEFTd6.h.

◆ CHL1_23i

double NPSMEFTd6::CHL1_23i
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).

Definition at line 4501 of file NPSMEFTd6.h.

◆ CHL1_23r

double NPSMEFTd6::CHL1_23r
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).

Definition at line 4497 of file NPSMEFTd6.h.

◆ CHL1_33

double NPSMEFTd6::CHL1_33
protected

The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).

Definition at line 4498 of file NPSMEFTd6.h.

◆ CHL3_11

double NPSMEFTd6::CHL3_11
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).

Definition at line 4502 of file NPSMEFTd6.h.

◆ CHL3_12i

double NPSMEFTd6::CHL3_12i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 4508 of file NPSMEFTd6.h.

◆ CHL3_12r

double NPSMEFTd6::CHL3_12r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).

Definition at line 4503 of file NPSMEFTd6.h.

◆ CHL3_13i

double NPSMEFTd6::CHL3_13i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 4509 of file NPSMEFTd6.h.

◆ CHL3_13r

double NPSMEFTd6::CHL3_13r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).

Definition at line 4504 of file NPSMEFTd6.h.

◆ CHL3_22

double NPSMEFTd6::CHL3_22
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).

Definition at line 4505 of file NPSMEFTd6.h.

◆ CHL3_23i

double NPSMEFTd6::CHL3_23i
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 4510 of file NPSMEFTd6.h.

◆ CHL3_23r

double NPSMEFTd6::CHL3_23r
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).

Definition at line 4506 of file NPSMEFTd6.h.

◆ CHL3_33

double NPSMEFTd6::CHL3_33
protected

The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).

Definition at line 4507 of file NPSMEFTd6.h.

◆ CHQ1_11

double NPSMEFTd6::CHQ1_11
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).

Definition at line 4520 of file NPSMEFTd6.h.

◆ CHQ1_12i

double NPSMEFTd6::CHQ1_12i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).

Definition at line 4526 of file NPSMEFTd6.h.

◆ CHQ1_12r

double NPSMEFTd6::CHQ1_12r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).

Definition at line 4521 of file NPSMEFTd6.h.

◆ CHQ1_13i

double NPSMEFTd6::CHQ1_13i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).

Definition at line 4527 of file NPSMEFTd6.h.

◆ CHQ1_13r

double NPSMEFTd6::CHQ1_13r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).

Definition at line 4522 of file NPSMEFTd6.h.

◆ CHQ1_22

double NPSMEFTd6::CHQ1_22
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).

Definition at line 4523 of file NPSMEFTd6.h.

◆ CHQ1_23i

double NPSMEFTd6::CHQ1_23i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).

Definition at line 4528 of file NPSMEFTd6.h.

◆ CHQ1_23r

double NPSMEFTd6::CHQ1_23r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).

Definition at line 4524 of file NPSMEFTd6.h.

◆ CHQ1_33

double NPSMEFTd6::CHQ1_33
protected

The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).

Definition at line 4525 of file NPSMEFTd6.h.

◆ CHQ3_11

double NPSMEFTd6::CHQ3_11
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).

Definition at line 4529 of file NPSMEFTd6.h.

◆ CHQ3_12i

double NPSMEFTd6::CHQ3_12i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).

Definition at line 4535 of file NPSMEFTd6.h.

◆ CHQ3_12r

double NPSMEFTd6::CHQ3_12r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).

Definition at line 4530 of file NPSMEFTd6.h.

◆ CHQ3_13i

double NPSMEFTd6::CHQ3_13i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).

Definition at line 4536 of file NPSMEFTd6.h.

◆ CHQ3_13r

double NPSMEFTd6::CHQ3_13r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).

Definition at line 4531 of file NPSMEFTd6.h.

◆ CHQ3_22

double NPSMEFTd6::CHQ3_22
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).

Definition at line 4532 of file NPSMEFTd6.h.

◆ CHQ3_23i

double NPSMEFTd6::CHQ3_23i
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).

Definition at line 4537 of file NPSMEFTd6.h.

◆ CHQ3_23r

double NPSMEFTd6::CHQ3_23r
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).

Definition at line 4533 of file NPSMEFTd6.h.

◆ CHQ3_33

double NPSMEFTd6::CHQ3_33
protected

The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).

Definition at line 4534 of file NPSMEFTd6.h.

◆ cHSM

double NPSMEFTd6::cHSM
protected

Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.

Definition at line 5024 of file NPSMEFTd6.h.

◆ CHu_11

double NPSMEFTd6::CHu_11
protected

The dimension-6 operator coefficient \((C_{Hu})_{11}\).

Definition at line 4538 of file NPSMEFTd6.h.

◆ CHu_12i

double NPSMEFTd6::CHu_12i
protected

The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part).

Definition at line 4544 of file NPSMEFTd6.h.

◆ CHu_12r

double NPSMEFTd6::CHu_12r
protected

The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part).

Definition at line 4539 of file NPSMEFTd6.h.

◆ CHu_13i

double NPSMEFTd6::CHu_13i
protected

The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part).

Definition at line 4545 of file NPSMEFTd6.h.

◆ CHu_13r

double NPSMEFTd6::CHu_13r
protected

The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part).

Definition at line 4540 of file NPSMEFTd6.h.

◆ CHu_22

double NPSMEFTd6::CHu_22
protected

The dimension-6 operator coefficient \((C_{Hu})_{22}\).

Definition at line 4541 of file NPSMEFTd6.h.

◆ CHu_23i

double NPSMEFTd6::CHu_23i
protected

The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part).

Definition at line 4546 of file NPSMEFTd6.h.

◆ CHu_23r

double NPSMEFTd6::CHu_23r
protected

The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part).

Definition at line 4542 of file NPSMEFTd6.h.

◆ CHu_33

double NPSMEFTd6::CHu_33
protected

The dimension-6 operator coefficient \((C_{Hu})_{33}\).

Definition at line 4543 of file NPSMEFTd6.h.

◆ CHud_11i

double NPSMEFTd6::CHud_11i
protected

The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part).

Definition at line 4562 of file NPSMEFTd6.h.

◆ CHud_11r

double NPSMEFTd6::CHud_11r
protected

The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part).

Definition at line 4556 of file NPSMEFTd6.h.

◆ CHud_12i

double NPSMEFTd6::CHud_12i
protected

The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part).

Definition at line 4563 of file NPSMEFTd6.h.

◆ CHud_12r

double NPSMEFTd6::CHud_12r
protected

The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part).

Definition at line 4557 of file NPSMEFTd6.h.

◆ CHud_13i

double NPSMEFTd6::CHud_13i
protected

The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part).

Definition at line 4564 of file NPSMEFTd6.h.

◆ CHud_13r

double NPSMEFTd6::CHud_13r
protected

The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part).

Definition at line 4558 of file NPSMEFTd6.h.

◆ CHud_22i

double NPSMEFTd6::CHud_22i
protected

The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part).

Definition at line 4565 of file NPSMEFTd6.h.

◆ CHud_22r

double NPSMEFTd6::CHud_22r
protected

The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part).

Definition at line 4559 of file NPSMEFTd6.h.

◆ CHud_23i

double NPSMEFTd6::CHud_23i
protected

The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part).

Definition at line 4566 of file NPSMEFTd6.h.

◆ CHud_23r

double NPSMEFTd6::CHud_23r
protected

The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part).

Definition at line 4560 of file NPSMEFTd6.h.

◆ CHud_33i

double NPSMEFTd6::CHud_33i
protected

The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part).

Definition at line 4567 of file NPSMEFTd6.h.

◆ CHud_33r

double NPSMEFTd6::CHud_33r
protected

The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part).

Definition at line 4561 of file NPSMEFTd6.h.

◆ CHW

double NPSMEFTd6::CHW
protected

The dimension-6 operator coefficient \(C_{HW}\).

Definition at line 4480 of file NPSMEFTd6.h.

◆ CHWB

double NPSMEFTd6::CHWB
protected

The dimension-6 operator coefficient \(C_{HWB}\).

Definition at line 4488 of file NPSMEFTd6.h.

◆ CHWHB_gaga

double NPSMEFTd6::CHWHB_gaga
protected

The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\).

Definition at line 4482 of file NPSMEFTd6.h.

◆ CHWHB_gagaorth

double NPSMEFTd6::CHWHB_gagaorth
protected

The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\).

Definition at line 4483 of file NPSMEFTd6.h.

◆ CidH_11r

double NPSMEFTd6::CidH_11r
protected

Definition at line 4974 of file NPSMEFTd6.h.

◆ CidH_22r

double NPSMEFTd6::CidH_22r
protected

Definition at line 4975 of file NPSMEFTd6.h.

◆ CidH_33r

double NPSMEFTd6::CidH_33r
protected

Definition at line 4976 of file NPSMEFTd6.h.

◆ CiDHB

double NPSMEFTd6::CiDHB
protected

Definition at line 4958 of file NPSMEFTd6.h.

◆ CiDHW

double NPSMEFTd6::CiDHW
protected

Definition at line 4959 of file NPSMEFTd6.h.

◆ CieH_11r

double NPSMEFTd6::CieH_11r
protected

Definition at line 4966 of file NPSMEFTd6.h.

◆ CieH_22r

double NPSMEFTd6::CieH_22r
protected

Definition at line 4967 of file NPSMEFTd6.h.

◆ CieH_33r

double NPSMEFTd6::CieH_33r
protected

Definition at line 4968 of file NPSMEFTd6.h.

◆ CiH

double NPSMEFTd6::CiH
protected

Definition at line 4964 of file NPSMEFTd6.h.

◆ CiHB

double NPSMEFTd6::CiHB
protected

Definition at line 4957 of file NPSMEFTd6.h.

◆ CiHbox

double NPSMEFTd6::CiHbox
protected

Definition at line 4962 of file NPSMEFTd6.h.

◆ CiHD

double NPSMEFTd6::CiHD
protected

Definition at line 4963 of file NPSMEFTd6.h.

◆ CiHd_11

double NPSMEFTd6::CiHd_11
protected

Definition at line 4950 of file NPSMEFTd6.h.

◆ CiHd_22

double NPSMEFTd6::CiHd_22
protected

Definition at line 4951 of file NPSMEFTd6.h.

◆ CiHd_33

double NPSMEFTd6::CiHd_33
protected

Definition at line 4952 of file NPSMEFTd6.h.

◆ CiHe_11

double NPSMEFTd6::CiHe_11
protected

Definition at line 4942 of file NPSMEFTd6.h.

◆ CiHe_22

double NPSMEFTd6::CiHe_22
protected

Definition at line 4943 of file NPSMEFTd6.h.

◆ CiHe_33

double NPSMEFTd6::CiHe_33
protected

Definition at line 4944 of file NPSMEFTd6.h.

◆ CiHL1_11

double NPSMEFTd6::CiHL1_11
protected

Definition at line 4928 of file NPSMEFTd6.h.

◆ CiHL1_22

double NPSMEFTd6::CiHL1_22
protected

Definition at line 4929 of file NPSMEFTd6.h.

◆ CiHL1_33

double NPSMEFTd6::CiHL1_33
protected

Definition at line 4930 of file NPSMEFTd6.h.

◆ CiHL3_11

double NPSMEFTd6::CiHL3_11
protected

Definition at line 4931 of file NPSMEFTd6.h.

◆ CiHL3_22

double NPSMEFTd6::CiHL3_22
protected

Definition at line 4932 of file NPSMEFTd6.h.

◆ CiHL3_33

double NPSMEFTd6::CiHL3_33
protected

Definition at line 4933 of file NPSMEFTd6.h.

◆ CiHQ1_11

double NPSMEFTd6::CiHQ1_11
protected

Definition at line 4935 of file NPSMEFTd6.h.

◆ CiHQ1_22

double NPSMEFTd6::CiHQ1_22
protected

Definition at line 4936 of file NPSMEFTd6.h.

◆ CiHQ1_33

double NPSMEFTd6::CiHQ1_33
protected

Definition at line 4937 of file NPSMEFTd6.h.

◆ CiHQ3_11

double NPSMEFTd6::CiHQ3_11
protected

Definition at line 4938 of file NPSMEFTd6.h.

◆ CiHQ3_22

double NPSMEFTd6::CiHQ3_22
protected

Definition at line 4939 of file NPSMEFTd6.h.

◆ CiHQ3_33

double NPSMEFTd6::CiHQ3_33
protected

Definition at line 4940 of file NPSMEFTd6.h.

◆ CiHu_11

double NPSMEFTd6::CiHu_11
protected

Definition at line 4946 of file NPSMEFTd6.h.

◆ CiHu_22

double NPSMEFTd6::CiHu_22
protected

Definition at line 4947 of file NPSMEFTd6.h.

◆ CiHu_33

double NPSMEFTd6::CiHu_33
protected

Definition at line 4948 of file NPSMEFTd6.h.

◆ CiHW

double NPSMEFTd6::CiHW
protected

Definition at line 4956 of file NPSMEFTd6.h.

◆ CiHWB

double NPSMEFTd6::CiHWB
protected

Definition at line 4960 of file NPSMEFTd6.h.

◆ CiLL_1221

double NPSMEFTd6::CiLL_1221
protected

Definition at line 4990 of file NPSMEFTd6.h.

◆ CiLL_2112

double NPSMEFTd6::CiLL_2112
protected

Definition at line 4991 of file NPSMEFTd6.h.

◆ CiuB_11r

double NPSMEFTd6::CiuB_11r
protected

Definition at line 4986 of file NPSMEFTd6.h.

◆ CiuB_22r

double NPSMEFTd6::CiuB_22r
protected

Definition at line 4987 of file NPSMEFTd6.h.

◆ CiuB_33r

double NPSMEFTd6::CiuB_33r
protected

Definition at line 4988 of file NPSMEFTd6.h.

◆ CiuG_11r

double NPSMEFTd6::CiuG_11r
protected

Definition at line 4978 of file NPSMEFTd6.h.

◆ CiuG_22r

double NPSMEFTd6::CiuG_22r
protected

Definition at line 4979 of file NPSMEFTd6.h.

◆ CiuG_33r

double NPSMEFTd6::CiuG_33r
protected

Definition at line 4980 of file NPSMEFTd6.h.

◆ CiuH_11r

double NPSMEFTd6::CiuH_11r
protected

Definition at line 4970 of file NPSMEFTd6.h.

◆ CiuH_22r

double NPSMEFTd6::CiuH_22r
protected

Definition at line 4971 of file NPSMEFTd6.h.

◆ CiuH_33r

double NPSMEFTd6::CiuH_33r
protected

Definition at line 4972 of file NPSMEFTd6.h.

◆ CiuW_11r

double NPSMEFTd6::CiuW_11r
protected

Definition at line 4982 of file NPSMEFTd6.h.

◆ CiuW_22r

double NPSMEFTd6::CiuW_22r
protected

Definition at line 4983 of file NPSMEFTd6.h.

◆ CiuW_33r

double NPSMEFTd6::CiuW_33r
protected

Definition at line 4984 of file NPSMEFTd6.h.

◆ CiW

double NPSMEFTd6::CiW
protected

Definition at line 4954 of file NPSMEFTd6.h.

◆ CLd_1111

double NPSMEFTd6::CLd_1111
protected

Definition at line 4732 of file NPSMEFTd6.h.

◆ CLd_1122

double NPSMEFTd6::CLd_1122
protected

Definition at line 4733 of file NPSMEFTd6.h.

◆ CLd_1123

double NPSMEFTd6::CLd_1123
protected

Definition at line 4735 of file NPSMEFTd6.h.

◆ CLd_1132

double NPSMEFTd6::CLd_1132
protected

Definition at line 4736 of file NPSMEFTd6.h.

◆ CLd_1133

double NPSMEFTd6::CLd_1133
protected

Definition at line 4734 of file NPSMEFTd6.h.

◆ CLd_2211

double NPSMEFTd6::CLd_2211
protected

Definition at line 4733 of file NPSMEFTd6.h.

◆ CLd_2223

double NPSMEFTd6::CLd_2223
protected

Definition at line 4735 of file NPSMEFTd6.h.

◆ CLd_2232

double NPSMEFTd6::CLd_2232
protected

Definition at line 4736 of file NPSMEFTd6.h.

◆ CLd_3311

double NPSMEFTd6::CLd_3311
protected

Definition at line 4734 of file NPSMEFTd6.h.

◆ CLd_3323

double NPSMEFTd6::CLd_3323
protected

Definition at line 4735 of file NPSMEFTd6.h.

◆ CLd_3332

double NPSMEFTd6::CLd_3332
protected

Definition at line 4736 of file NPSMEFTd6.h.

◆ CLe_1111

double NPSMEFTd6::CLe_1111
protected

Definition at line 4725 of file NPSMEFTd6.h.

◆ CLe_1122

double NPSMEFTd6::CLe_1122
protected

Definition at line 4726 of file NPSMEFTd6.h.

◆ CLe_1133

double NPSMEFTd6::CLe_1133
protected

Definition at line 4727 of file NPSMEFTd6.h.

◆ CLe_2211

double NPSMEFTd6::CLe_2211
protected

Definition at line 4726 of file NPSMEFTd6.h.

◆ CLe_3311

double NPSMEFTd6::CLe_3311
protected

Definition at line 4727 of file NPSMEFTd6.h.

◆ CLedQ_11

double NPSMEFTd6::CLedQ_11
protected

Definition at line 4742 of file NPSMEFTd6.h.

◆ CLedQ_22

double NPSMEFTd6::CLedQ_22
protected

Definition at line 4742 of file NPSMEFTd6.h.

◆ cLH3d62

double NPSMEFTd6::cLH3d62
protected

Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms).

Definition at line 5028 of file NPSMEFTd6.h.

◆ cLHd6

double NPSMEFTd6::cLHd6
protected

Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions.

Definition at line 5026 of file NPSMEFTd6.h.

◆ CLL_1111

double NPSMEFTd6::CLL_1111
protected

Definition at line 4700 of file NPSMEFTd6.h.

◆ CLL_1122

double NPSMEFTd6::CLL_1122
protected

Definition at line 4701 of file NPSMEFTd6.h.

◆ CLL_1133

double NPSMEFTd6::CLL_1133
protected

Definition at line 4702 of file NPSMEFTd6.h.

◆ CLL_1221

double NPSMEFTd6::CLL_1221
protected

Definition at line 4701 of file NPSMEFTd6.h.

◆ CLL_1331

double NPSMEFTd6::CLL_1331
protected

Definition at line 4702 of file NPSMEFTd6.h.

◆ CLL_2112

double NPSMEFTd6::CLL_2112
protected

Definition at line 4701 of file NPSMEFTd6.h.

◆ CLL_2211

double NPSMEFTd6::CLL_2211
protected

Definition at line 4701 of file NPSMEFTd6.h.

◆ CLL_3113

double NPSMEFTd6::CLL_3113
protected

Definition at line 4702 of file NPSMEFTd6.h.

◆ CLL_3311

double NPSMEFTd6::CLL_3311
protected

Definition at line 4702 of file NPSMEFTd6.h.

◆ CLQ1_1111

double NPSMEFTd6::CLQ1_1111
protected

Definition at line 4703 of file NPSMEFTd6.h.

◆ CLQ1_1122

double NPSMEFTd6::CLQ1_1122
protected

Definition at line 4704 of file NPSMEFTd6.h.

◆ CLQ1_1123

double NPSMEFTd6::CLQ1_1123
protected

Definition at line 4706 of file NPSMEFTd6.h.

◆ CLQ1_1132

double NPSMEFTd6::CLQ1_1132
protected

Definition at line 4707 of file NPSMEFTd6.h.

◆ CLQ1_1133

double NPSMEFTd6::CLQ1_1133
protected

Definition at line 4705 of file NPSMEFTd6.h.

◆ CLQ1_1221

double NPSMEFTd6::CLQ1_1221
protected

Definition at line 4704 of file NPSMEFTd6.h.

◆ CLQ1_1331

double NPSMEFTd6::CLQ1_1331
protected

Definition at line 4705 of file NPSMEFTd6.h.

◆ CLQ1_2112

double NPSMEFTd6::CLQ1_2112
protected

Definition at line 4704 of file NPSMEFTd6.h.

◆ CLQ1_2211

double NPSMEFTd6::CLQ1_2211
protected

Definition at line 4704 of file NPSMEFTd6.h.

◆ CLQ1_2223

double NPSMEFTd6::CLQ1_2223
protected

Definition at line 4706 of file NPSMEFTd6.h.

◆ CLQ1_2232

double NPSMEFTd6::CLQ1_2232
protected

Definition at line 4707 of file NPSMEFTd6.h.

◆ CLQ1_3113

double NPSMEFTd6::CLQ1_3113
protected

Definition at line 4705 of file NPSMEFTd6.h.

◆ CLQ1_3311

double NPSMEFTd6::CLQ1_3311
protected

Definition at line 4705 of file NPSMEFTd6.h.

◆ CLQ1_3323

double NPSMEFTd6::CLQ1_3323
protected

Definition at line 4706 of file NPSMEFTd6.h.

◆ CLQ1_3332

double NPSMEFTd6::CLQ1_3332
protected

Definition at line 4707 of file NPSMEFTd6.h.

◆ CLQ3_1111

double NPSMEFTd6::CLQ3_1111
protected

Definition at line 4708 of file NPSMEFTd6.h.

◆ CLQ3_1122

double NPSMEFTd6::CLQ3_1122
protected

Definition at line 4709 of file NPSMEFTd6.h.

◆ CLQ3_1123

double NPSMEFTd6::CLQ3_1123
protected

Definition at line 4711 of file NPSMEFTd6.h.

◆ CLQ3_1132

double NPSMEFTd6::CLQ3_1132
protected

Definition at line 4712 of file NPSMEFTd6.h.

◆ CLQ3_1133

double NPSMEFTd6::CLQ3_1133
protected

Definition at line 4710 of file NPSMEFTd6.h.

◆ CLQ3_1221

double NPSMEFTd6::CLQ3_1221
protected

Definition at line 4709 of file NPSMEFTd6.h.

◆ CLQ3_1331

double NPSMEFTd6::CLQ3_1331
protected

Definition at line 4710 of file NPSMEFTd6.h.

◆ CLQ3_2112

double NPSMEFTd6::CLQ3_2112
protected

Definition at line 4709 of file NPSMEFTd6.h.

◆ CLQ3_2211

double NPSMEFTd6::CLQ3_2211
protected

Definition at line 4709 of file NPSMEFTd6.h.

◆ CLQ3_2223

double NPSMEFTd6::CLQ3_2223
protected

Definition at line 4711 of file NPSMEFTd6.h.

◆ CLQ3_2232

double NPSMEFTd6::CLQ3_2232
protected

Definition at line 4712 of file NPSMEFTd6.h.

◆ CLQ3_3113

double NPSMEFTd6::CLQ3_3113
protected

Definition at line 4710 of file NPSMEFTd6.h.

◆ CLQ3_3311

double NPSMEFTd6::CLQ3_3311
protected

Definition at line 4710 of file NPSMEFTd6.h.

◆ CLQ3_3323

double NPSMEFTd6::CLQ3_3323
protected

Definition at line 4711 of file NPSMEFTd6.h.

◆ CLQ3_3332

double NPSMEFTd6::CLQ3_3332
protected

Definition at line 4712 of file NPSMEFTd6.h.

◆ CLu_1111

double NPSMEFTd6::CLu_1111
protected

Definition at line 4728 of file NPSMEFTd6.h.

◆ CLu_1122

double NPSMEFTd6::CLu_1122
protected

Definition at line 4729 of file NPSMEFTd6.h.

◆ CLu_1133

double NPSMEFTd6::CLu_1133
protected

Definition at line 4730 of file NPSMEFTd6.h.

◆ CLu_2211

double NPSMEFTd6::CLu_2211
protected

Definition at line 4729 of file NPSMEFTd6.h.

◆ CLu_2233

double NPSMEFTd6::CLu_2233
protected

Definition at line 4731 of file NPSMEFTd6.h.

◆ CLu_3311

double NPSMEFTd6::CLu_3311
protected

Definition at line 4730 of file NPSMEFTd6.h.

◆ CpLedQ_11

double NPSMEFTd6::CpLedQ_11
protected

Definition at line 4742 of file NPSMEFTd6.h.

◆ CpLedQ_22

double NPSMEFTd6::CpLedQ_22
protected

Definition at line 4742 of file NPSMEFTd6.h.

◆ CQe_1111

double NPSMEFTd6::CQe_1111
protected

Definition at line 4737 of file NPSMEFTd6.h.

◆ CQe_1122

double NPSMEFTd6::CQe_1122
protected

Definition at line 4738 of file NPSMEFTd6.h.

◆ CQe_1133

double NPSMEFTd6::CQe_1133
protected

Definition at line 4739 of file NPSMEFTd6.h.

◆ CQe_2211

double NPSMEFTd6::CQe_2211
protected

Definition at line 4738 of file NPSMEFTd6.h.

◆ CQe_2311

double NPSMEFTd6::CQe_2311
protected

Definition at line 4740 of file NPSMEFTd6.h.

◆ CQe_2322

double NPSMEFTd6::CQe_2322
protected

Definition at line 4740 of file NPSMEFTd6.h.

◆ CQe_2333

double NPSMEFTd6::CQe_2333
protected

Definition at line 4740 of file NPSMEFTd6.h.

◆ CQe_3211

double NPSMEFTd6::CQe_3211
protected

Definition at line 4741 of file NPSMEFTd6.h.

◆ CQe_3222

double NPSMEFTd6::CQe_3222
protected

Definition at line 4741 of file NPSMEFTd6.h.

◆ CQe_3233

double NPSMEFTd6::CQe_3233
protected

Definition at line 4741 of file NPSMEFTd6.h.

◆ CQe_3311

double NPSMEFTd6::CQe_3311
protected

Definition at line 4739 of file NPSMEFTd6.h.

◆ CT

double NPSMEFTd6::CT
protected

The dimension-6 operator coefficient \(C_{T}\).

Definition at line 4490 of file NPSMEFTd6.h.

◆ CuB_11i

double NPSMEFTd6::CuB_11i
protected

The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part).

Definition at line 4634 of file NPSMEFTd6.h.

◆ CuB_11r

double NPSMEFTd6::CuB_11r
protected

The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part).

Definition at line 4628 of file NPSMEFTd6.h.

◆ CuB_12i

double NPSMEFTd6::CuB_12i
protected

The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part).

Definition at line 4635 of file NPSMEFTd6.h.

◆ CuB_12r

double NPSMEFTd6::CuB_12r
protected

The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part).

Definition at line 4629 of file NPSMEFTd6.h.

◆ CuB_13i

double NPSMEFTd6::CuB_13i
protected

The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part).

Definition at line 4636 of file NPSMEFTd6.h.

◆ CuB_13r

double NPSMEFTd6::CuB_13r
protected

The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part).

Definition at line 4630 of file NPSMEFTd6.h.

◆ CuB_22i

double NPSMEFTd6::CuB_22i
protected

The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part).

Definition at line 4637 of file NPSMEFTd6.h.

◆ CuB_22r

double NPSMEFTd6::CuB_22r
protected

The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part).

Definition at line 4631 of file NPSMEFTd6.h.

◆ CuB_23i

double NPSMEFTd6::CuB_23i
protected

The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part).

Definition at line 4638 of file NPSMEFTd6.h.

◆ CuB_23r

double NPSMEFTd6::CuB_23r
protected

The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part).

Definition at line 4632 of file NPSMEFTd6.h.

◆ CuB_33i

double NPSMEFTd6::CuB_33i
protected

The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part).

Definition at line 4639 of file NPSMEFTd6.h.

◆ CuB_33r

double NPSMEFTd6::CuB_33r
protected

The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part).

Definition at line 4633 of file NPSMEFTd6.h.

◆ CuG_11i

double NPSMEFTd6::CuG_11i
protected

The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part).

Definition at line 4610 of file NPSMEFTd6.h.

◆ CuG_11r

double NPSMEFTd6::CuG_11r
protected

The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part).

Definition at line 4604 of file NPSMEFTd6.h.

◆ CuG_12i

double NPSMEFTd6::CuG_12i
protected

The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part).

Definition at line 4611 of file NPSMEFTd6.h.

◆ CuG_12r

double NPSMEFTd6::CuG_12r
protected

The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part).

Definition at line 4605 of file NPSMEFTd6.h.

◆ CuG_13i

double NPSMEFTd6::CuG_13i
protected

The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part).

Definition at line 4612 of file NPSMEFTd6.h.

◆ CuG_13r

double NPSMEFTd6::CuG_13r
protected

The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part).

Definition at line 4606 of file NPSMEFTd6.h.

◆ CuG_22i

double NPSMEFTd6::CuG_22i
protected

The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part).

Definition at line 4613 of file NPSMEFTd6.h.

◆ CuG_22r

double NPSMEFTd6::CuG_22r
protected

The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part).

Definition at line 4607 of file NPSMEFTd6.h.

◆ CuG_23i

double NPSMEFTd6::CuG_23i
protected

The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part).

Definition at line 4614 of file NPSMEFTd6.h.

◆ CuG_23r

double NPSMEFTd6::CuG_23r
protected

The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part).

Definition at line 4608 of file NPSMEFTd6.h.

◆ CuG_33i

double NPSMEFTd6::CuG_33i
protected

The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part).

Definition at line 4615 of file NPSMEFTd6.h.

◆ CuG_33r

double NPSMEFTd6::CuG_33r
protected

The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part).

Definition at line 4609 of file NPSMEFTd6.h.

◆ CuH_11i

double NPSMEFTd6::CuH_11i
protected

The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part).

Definition at line 4586 of file NPSMEFTd6.h.

◆ CuH_11r

double NPSMEFTd6::CuH_11r
protected

The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part).

Definition at line 4580 of file NPSMEFTd6.h.

◆ CuH_12i

double NPSMEFTd6::CuH_12i
protected

The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part).

Definition at line 4587 of file NPSMEFTd6.h.

◆ CuH_12r

double NPSMEFTd6::CuH_12r
protected

The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part).

Definition at line 4581 of file NPSMEFTd6.h.

◆ CuH_13i

double NPSMEFTd6::CuH_13i
protected

The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part).

Definition at line 4588 of file NPSMEFTd6.h.

◆ CuH_13r

double NPSMEFTd6::CuH_13r
protected

The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part).

Definition at line 4582 of file NPSMEFTd6.h.

◆ CuH_22i

double NPSMEFTd6::CuH_22i
protected

The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part).

Definition at line 4589 of file NPSMEFTd6.h.

◆ CuH_22r

double NPSMEFTd6::CuH_22r
protected

The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part).

Definition at line 4583 of file NPSMEFTd6.h.

◆ CuH_23i

double NPSMEFTd6::CuH_23i
protected

The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part).

Definition at line 4590 of file NPSMEFTd6.h.

◆ CuH_23r

double NPSMEFTd6::CuH_23r
protected

The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part).

Definition at line 4584 of file NPSMEFTd6.h.

◆ CuH_33i

double NPSMEFTd6::CuH_33i
protected

The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part).

Definition at line 4591 of file NPSMEFTd6.h.

◆ CuH_33r

double NPSMEFTd6::CuH_33r
protected

The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part).

Definition at line 4585 of file NPSMEFTd6.h.

◆ CuW_11i

double NPSMEFTd6::CuW_11i
protected

The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part).

Definition at line 4622 of file NPSMEFTd6.h.

◆ CuW_11r

double NPSMEFTd6::CuW_11r
protected

The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part).

Definition at line 4616 of file NPSMEFTd6.h.

◆ CuW_12i

double NPSMEFTd6::CuW_12i
protected

The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part).

Definition at line 4623 of file NPSMEFTd6.h.

◆ CuW_12r

double NPSMEFTd6::CuW_12r
protected

The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part).

Definition at line 4617 of file NPSMEFTd6.h.

◆ CuW_13i

double NPSMEFTd6::CuW_13i
protected

The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part).

Definition at line 4624 of file NPSMEFTd6.h.

◆ CuW_13r

double NPSMEFTd6::CuW_13r
protected

The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part).

Definition at line 4618 of file NPSMEFTd6.h.

◆ CuW_22i

double NPSMEFTd6::CuW_22i
protected

The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part).

Definition at line 4625 of file NPSMEFTd6.h.

◆ CuW_22r

double NPSMEFTd6::CuW_22r
protected

The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part).

Definition at line 4619 of file NPSMEFTd6.h.

◆ CuW_23i

double NPSMEFTd6::CuW_23i
protected

The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part).

Definition at line 4626 of file NPSMEFTd6.h.

◆ CuW_23r

double NPSMEFTd6::CuW_23r
protected

The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part).

Definition at line 4620 of file NPSMEFTd6.h.

◆ CuW_33i

double NPSMEFTd6::CuW_33i
protected

The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part).

Definition at line 4627 of file NPSMEFTd6.h.

◆ CuW_33r

double NPSMEFTd6::CuW_33r
protected

The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part).

Definition at line 4621 of file NPSMEFTd6.h.

◆ CW

double NPSMEFTd6::CW
protected

The dimension-6 operator coefficient \(C_{W}\).

Definition at line 4474 of file NPSMEFTd6.h.

◆ cW2_tree

double NPSMEFTd6::cW2_tree
protected

The square of the tree level values for the cosine of the weak angle.

Definition at line 5000 of file NPSMEFTd6.h.

◆ cW_tree

double NPSMEFTd6::cW_tree
protected

The tree level values for the cosine of the weak angle.

Definition at line 4998 of file NPSMEFTd6.h.

◆ delta_AA

double NPSMEFTd6::delta_AA
protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 5016 of file NPSMEFTd6.h.

◆ delta_AZ

double NPSMEFTd6::delta_AZ
protected

Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.

Definition at line 5017 of file NPSMEFTd6.h.

◆ delta_h

double NPSMEFTd6::delta_h
protected

Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.

Definition at line 5018 of file NPSMEFTd6.h.

◆ delta_ZZ

double NPSMEFTd6::delta_ZZ
protected

Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.

Definition at line 5015 of file NPSMEFTd6.h.

◆ dg1Z

double NPSMEFTd6::dg1Z
protected

Independent contribution to aTGC.

Definition at line 4917 of file NPSMEFTd6.h.

◆ dGammaHTotR1

double NPSMEFTd6::dGammaHTotR1
protected

Definition at line 5042 of file NPSMEFTd6.h.

◆ dGammaHTotR2

double NPSMEFTd6::dGammaHTotR2
protected

Definition at line 5042 of file NPSMEFTd6.h.

◆ dKappaga

double NPSMEFTd6::dKappaga
protected

Independent contribution to aTGC.

Definition at line 4918 of file NPSMEFTd6.h.

◆ dZH

double NPSMEFTd6::dZH
protected

Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.

Definition at line 5022 of file NPSMEFTd6.h.

◆ eeettHint

double NPSMEFTd6::eeettHint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)

Definition at line 4759 of file NPSMEFTd6.h.

◆ eeettHpar

double NPSMEFTd6::eeettHpar
protected

Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)

Definition at line 4760 of file NPSMEFTd6.h.

◆ eeeWBFint

double NPSMEFTd6::eeeWBFint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)

Definition at line 4755 of file NPSMEFTd6.h.

◆ eeeWBFpar

double NPSMEFTd6::eeeWBFpar
protected

Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)

Definition at line 4756 of file NPSMEFTd6.h.

◆ eeeZHint

double NPSMEFTd6::eeeZHint
protected

Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)

Definition at line 4757 of file NPSMEFTd6.h.

◆ eeeZHpar

double NPSMEFTd6::eeeZHpar
protected

Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)

Definition at line 4758 of file NPSMEFTd6.h.

◆ eeMz

double NPSMEFTd6::eeMz
protected

The em coupling at Mz.

Definition at line 4996 of file NPSMEFTd6.h.

◆ eeMz2

double NPSMEFTd6::eeMz2
protected

The em coupling squared (at Mz).

Definition at line 4997 of file NPSMEFTd6.h.

◆ eepWBFint

double NPSMEFTd6::eepWBFint
protected

Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)

Definition at line 4761 of file NPSMEFTd6.h.

◆ eepWBFpar

double NPSMEFTd6::eepWBFpar
protected

Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)

Definition at line 4762 of file NPSMEFTd6.h.

◆ eepZBFint

double NPSMEFTd6::eepZBFint
protected

Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)

Definition at line 4763 of file NPSMEFTd6.h.

◆ eepZBFpar

double NPSMEFTd6::eepZBFpar
protected

Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)

Definition at line 4764 of file NPSMEFTd6.h.

◆ eggFHbb

double NPSMEFTd6::eggFHbb
protected

Definition at line 4784 of file NPSMEFTd6.h.

◆ eggFHgaga

double NPSMEFTd6::eggFHgaga
protected

Definition at line 4784 of file NPSMEFTd6.h.

◆ eggFHmumu

double NPSMEFTd6::eggFHmumu
protected

Total relative theoretical error in \(gg \to H \to X\).

Definition at line 4784 of file NPSMEFTd6.h.

◆ eggFHtautau

double NPSMEFTd6::eggFHtautau
protected

Definition at line 4784 of file NPSMEFTd6.h.

◆ eggFHWW

double NPSMEFTd6::eggFHWW
protected

Definition at line 4784 of file NPSMEFTd6.h.

◆ eggFHZga

double NPSMEFTd6::eggFHZga
protected

Definition at line 4784 of file NPSMEFTd6.h.

◆ eggFHZZ

double NPSMEFTd6::eggFHZZ
protected

Definition at line 4784 of file NPSMEFTd6.h.

◆ eggFint

double NPSMEFTd6::eggFint
protected

Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.)

Definition at line 4745 of file NPSMEFTd6.h.

◆ eggFpar

double NPSMEFTd6::eggFpar
protected

Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.)

Definition at line 4746 of file NPSMEFTd6.h.

◆ eHbbint

double NPSMEFTd6::eHbbint
protected

Intrinsic relative theoretical error in \(H \to b\bar{b}\).

Definition at line 4781 of file NPSMEFTd6.h.

◆ eHbbpar

double NPSMEFTd6::eHbbpar
protected

Parametric relative theoretical error in \(H \to b\bar{b}\).

Definition at line 4782 of file NPSMEFTd6.h.

◆ eHccint

double NPSMEFTd6::eHccint
protected

Intrinsic relative theoretical error in \(H \to c\bar{c}\).

Definition at line 4779 of file NPSMEFTd6.h.

◆ eHccpar

double NPSMEFTd6::eHccpar
protected

Parametric relative theoretical error in \(H \to c\bar{c}\).

Definition at line 4780 of file NPSMEFTd6.h.

◆ eHgagaint

double NPSMEFTd6::eHgagaint
protected

Intrinsic relative theoretical error in \(H \to \gamma\gamma\).

Definition at line 4773 of file NPSMEFTd6.h.

◆ eHgagapar

double NPSMEFTd6::eHgagapar
protected

Parametric relative theoretical error in \(H \to \gamma\gamma\).

Definition at line 4774 of file NPSMEFTd6.h.

◆ eHggint

double NPSMEFTd6::eHggint
protected

Intrinsic relative theoretical error in \(H \to g g\).

Definition at line 4765 of file NPSMEFTd6.h.

◆ eHggpar

double NPSMEFTd6::eHggpar
protected

Parametric relative theoretical error in \(H \to g g\).

Definition at line 4766 of file NPSMEFTd6.h.

◆ eHmumuint

double NPSMEFTd6::eHmumuint
protected

Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\).

Definition at line 4775 of file NPSMEFTd6.h.

◆ eHmumupar

double NPSMEFTd6::eHmumupar
protected

Parametric relative theoretical error in \(H \to \mu^+ \mu^-\).

Definition at line 4776 of file NPSMEFTd6.h.

◆ eHtautauint

double NPSMEFTd6::eHtautauint
protected

Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\).

Definition at line 4777 of file NPSMEFTd6.h.

◆ eHtautaupar

double NPSMEFTd6::eHtautaupar
protected

Parametric relative theoretical error in \(H \to \tau^+ \tau^-\).

Definition at line 4778 of file NPSMEFTd6.h.

◆ eHwidth

double NPSMEFTd6::eHwidth
protected

Total relative theoretical error in the Higgs width.

Definition at line 4791 of file NPSMEFTd6.h.

◆ eHWWint

double NPSMEFTd6::eHWWint
protected

Intrinsic relative theoretical error in \(H \to W W\).

Definition at line 4767 of file NPSMEFTd6.h.

◆ eHWWpar

double NPSMEFTd6::eHWWpar
protected

Parametric relative theoretical error in \(H \to W W\).

Definition at line 4768 of file NPSMEFTd6.h.

◆ eHZgaint

double NPSMEFTd6::eHZgaint
protected

Intrinsic relative theoretical error in \(H \to Z \gamma\).

Definition at line 4771 of file NPSMEFTd6.h.

◆ eHZgapar

double NPSMEFTd6::eHZgapar
protected

Parametric relative theoretical error in \(H \to Z \gamma\).

Definition at line 4772 of file NPSMEFTd6.h.

◆ eHZZint

double NPSMEFTd6::eHZZint
protected

Intrinsic relative theoretical error in \(H \to Z Z\).

Definition at line 4769 of file NPSMEFTd6.h.

◆ eHZZpar

double NPSMEFTd6::eHZZpar
protected

Parametric relative theoretical error in \(H \to Z Z\).

Definition at line 4770 of file NPSMEFTd6.h.

◆ ettH_1314_DeltagHt

double NPSMEFTd6::ettH_1314_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV).

Definition at line 4912 of file NPSMEFTd6.h.

◆ ettH_1314_G

double NPSMEFTd6::ettH_1314_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV).

Definition at line 4910 of file NPSMEFTd6.h.

◆ ettH_1314_HG

double NPSMEFTd6::ettH_1314_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV).

Definition at line 4909 of file NPSMEFTd6.h.

◆ ettH_1314_uG_33r

double NPSMEFTd6::ettH_1314_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV).

Definition at line 4911 of file NPSMEFTd6.h.

◆ ettH_2_DeltagHt

double NPSMEFTd6::ettH_2_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV).

Definition at line 4902 of file NPSMEFTd6.h.

◆ ettH_2_G

double NPSMEFTd6::ettH_2_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 4900 of file NPSMEFTd6.h.

◆ ettH_2_HG

double NPSMEFTd6::ettH_2_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV).

Definition at line 4899 of file NPSMEFTd6.h.

◆ ettH_2_uG_33r

double NPSMEFTd6::ettH_2_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV).

Definition at line 4901 of file NPSMEFTd6.h.

◆ ettH_78_DeltagHt

double NPSMEFTd6::ettH_78_DeltagHt
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 4907 of file NPSMEFTd6.h.

◆ ettH_78_G

double NPSMEFTd6::ettH_78_G
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV).

Definition at line 4905 of file NPSMEFTd6.h.

◆ ettH_78_HG

double NPSMEFTd6::ettH_78_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV).

Definition at line 4904 of file NPSMEFTd6.h.

◆ ettH_78_uG_33r

double NPSMEFTd6::ettH_78_uG_33r
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV).

Definition at line 4906 of file NPSMEFTd6.h.

◆ ettHbb

double NPSMEFTd6::ettHbb
protected

Definition at line 4788 of file NPSMEFTd6.h.

◆ ettHgaga

double NPSMEFTd6::ettHgaga
protected

Definition at line 4788 of file NPSMEFTd6.h.

◆ ettHint

double NPSMEFTd6::ettHint
protected

Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.)

Definition at line 4747 of file NPSMEFTd6.h.

◆ ettHmumu

double NPSMEFTd6::ettHmumu
protected

Total relative theoretical error in \(pp \to ttH \to tt X\).

Definition at line 4788 of file NPSMEFTd6.h.

◆ ettHpar

double NPSMEFTd6::ettHpar
protected

Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.)

Definition at line 4748 of file NPSMEFTd6.h.

◆ ettHtautau

double NPSMEFTd6::ettHtautau
protected

Definition at line 4788 of file NPSMEFTd6.h.

◆ ettHWW

double NPSMEFTd6::ettHWW
protected

Definition at line 4788 of file NPSMEFTd6.h.

◆ ettHZga

double NPSMEFTd6::ettHZga
protected

Definition at line 4788 of file NPSMEFTd6.h.

◆ ettHZZ

double NPSMEFTd6::ettHZZ
protected

Definition at line 4788 of file NPSMEFTd6.h.

◆ eVBF_1314_DeltaGF

double NPSMEFTd6::eVBF_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4834 of file NPSMEFTd6.h.

◆ eVBF_1314_DHB

double NPSMEFTd6::eVBF_1314_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4832 of file NPSMEFTd6.h.

◆ eVBF_1314_DHW

double NPSMEFTd6::eVBF_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4833 of file NPSMEFTd6.h.

◆ eVBF_1314_HB

double NPSMEFTd6::eVBF_1314_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4828 of file NPSMEFTd6.h.

◆ eVBF_1314_Hbox

double NPSMEFTd6::eVBF_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4822 of file NPSMEFTd6.h.

◆ eVBF_1314_HD

double NPSMEFTd6::eVBF_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4827 of file NPSMEFTd6.h.

◆ eVBF_1314_Hd_11

double NPSMEFTd6::eVBF_1314_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4825 of file NPSMEFTd6.h.

◆ eVBF_1314_HG

double NPSMEFTd6::eVBF_1314_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4831 of file NPSMEFTd6.h.

◆ eVBF_1314_HQ1_11

double NPSMEFTd6::eVBF_1314_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4823 of file NPSMEFTd6.h.

◆ eVBF_1314_HQ3_11

double NPSMEFTd6::eVBF_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4826 of file NPSMEFTd6.h.

◆ eVBF_1314_Hu_11

double NPSMEFTd6::eVBF_1314_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4824 of file NPSMEFTd6.h.

◆ eVBF_1314_HW

double NPSMEFTd6::eVBF_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4829 of file NPSMEFTd6.h.

◆ eVBF_1314_HWB

double NPSMEFTd6::eVBF_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV).

Definition at line 4830 of file NPSMEFTd6.h.

◆ eVBF_2_DeltaGF

double NPSMEFTd6::eVBF_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4806 of file NPSMEFTd6.h.

◆ eVBF_2_DHB

double NPSMEFTd6::eVBF_2_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4804 of file NPSMEFTd6.h.

◆ eVBF_2_DHW

double NPSMEFTd6::eVBF_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4805 of file NPSMEFTd6.h.

◆ eVBF_2_HB

double NPSMEFTd6::eVBF_2_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4800 of file NPSMEFTd6.h.

◆ eVBF_2_Hbox

double NPSMEFTd6::eVBF_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4794 of file NPSMEFTd6.h.

◆ eVBF_2_HD

double NPSMEFTd6::eVBF_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4799 of file NPSMEFTd6.h.

◆ eVBF_2_Hd_11

double NPSMEFTd6::eVBF_2_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4797 of file NPSMEFTd6.h.

◆ eVBF_2_HG

double NPSMEFTd6::eVBF_2_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4803 of file NPSMEFTd6.h.

◆ eVBF_2_HQ1_11

double NPSMEFTd6::eVBF_2_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4795 of file NPSMEFTd6.h.

◆ eVBF_2_HQ3_11

double NPSMEFTd6::eVBF_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4798 of file NPSMEFTd6.h.

◆ eVBF_2_Hu_11

double NPSMEFTd6::eVBF_2_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4796 of file NPSMEFTd6.h.

◆ eVBF_2_HW

double NPSMEFTd6::eVBF_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4801 of file NPSMEFTd6.h.

◆ eVBF_2_HWB

double NPSMEFTd6::eVBF_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV).

Definition at line 4802 of file NPSMEFTd6.h.

◆ eVBF_78_DeltaGF

double NPSMEFTd6::eVBF_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4820 of file NPSMEFTd6.h.

◆ eVBF_78_DHB

double NPSMEFTd6::eVBF_78_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4818 of file NPSMEFTd6.h.

◆ eVBF_78_DHW

double NPSMEFTd6::eVBF_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4819 of file NPSMEFTd6.h.

◆ eVBF_78_HB

double NPSMEFTd6::eVBF_78_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4814 of file NPSMEFTd6.h.

◆ eVBF_78_Hbox

double NPSMEFTd6::eVBF_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4808 of file NPSMEFTd6.h.

◆ eVBF_78_HD

double NPSMEFTd6::eVBF_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4813 of file NPSMEFTd6.h.

◆ eVBF_78_Hd_11

double NPSMEFTd6::eVBF_78_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4811 of file NPSMEFTd6.h.

◆ eVBF_78_HG

double NPSMEFTd6::eVBF_78_HG
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4817 of file NPSMEFTd6.h.

◆ eVBF_78_HQ1_11

double NPSMEFTd6::eVBF_78_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4809 of file NPSMEFTd6.h.

◆ eVBF_78_HQ3_11

double NPSMEFTd6::eVBF_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4812 of file NPSMEFTd6.h.

◆ eVBF_78_Hu_11

double NPSMEFTd6::eVBF_78_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4810 of file NPSMEFTd6.h.

◆ eVBF_78_HW

double NPSMEFTd6::eVBF_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4815 of file NPSMEFTd6.h.

◆ eVBF_78_HWB

double NPSMEFTd6::eVBF_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV).

Definition at line 4816 of file NPSMEFTd6.h.

◆ eVBFHbb

double NPSMEFTd6::eVBFHbb
protected

Definition at line 4785 of file NPSMEFTd6.h.

◆ eVBFHgaga

double NPSMEFTd6::eVBFHgaga
protected

Definition at line 4785 of file NPSMEFTd6.h.

◆ eVBFHinv

double NPSMEFTd6::eVBFHinv
protected

Definition at line 4789 of file NPSMEFTd6.h.

◆ eVBFHmumu

double NPSMEFTd6::eVBFHmumu
protected

Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).

Definition at line 4785 of file NPSMEFTd6.h.

◆ eVBFHtautau

double NPSMEFTd6::eVBFHtautau
protected

Definition at line 4785 of file NPSMEFTd6.h.

◆ eVBFHWW

double NPSMEFTd6::eVBFHWW
protected

Definition at line 4785 of file NPSMEFTd6.h.

◆ eVBFHZga

double NPSMEFTd6::eVBFHZga
protected

Definition at line 4785 of file NPSMEFTd6.h.

◆ eVBFHZZ

double NPSMEFTd6::eVBFHZZ
protected

Definition at line 4785 of file NPSMEFTd6.h.

◆ eVBFint

double NPSMEFTd6::eVBFint
protected

Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.)

Definition at line 4749 of file NPSMEFTd6.h.

◆ eVBFpar

double NPSMEFTd6::eVBFpar
protected

Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.)

Definition at line 4750 of file NPSMEFTd6.h.

◆ eVHinv

double NPSMEFTd6::eVHinv
protected

Total relative theoretical error in \(pp \to X H \to X + invisible\).

Definition at line 4789 of file NPSMEFTd6.h.

◆ eWH_1314_DeltaGF

double NPSMEFTd6::eWH_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV).

Definition at line 4858 of file NPSMEFTd6.h.

◆ eWH_1314_DHW

double NPSMEFTd6::eWH_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV).

Definition at line 4857 of file NPSMEFTd6.h.

◆ eWH_1314_Hbox

double NPSMEFTd6::eWH_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4852 of file NPSMEFTd6.h.

◆ eWH_1314_HD

double NPSMEFTd6::eWH_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4854 of file NPSMEFTd6.h.

◆ eWH_1314_HQ3_11

double NPSMEFTd6::eWH_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4853 of file NPSMEFTd6.h.

◆ eWH_1314_HW

double NPSMEFTd6::eWH_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4855 of file NPSMEFTd6.h.

◆ eWH_1314_HWB

double NPSMEFTd6::eWH_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV).

Definition at line 4856 of file NPSMEFTd6.h.

◆ eWH_2_DeltaGF

double NPSMEFTd6::eWH_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV).

Definition at line 4842 of file NPSMEFTd6.h.

◆ eWH_2_DHW

double NPSMEFTd6::eWH_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV).

Definition at line 4841 of file NPSMEFTd6.h.

◆ eWH_2_Hbox

double NPSMEFTd6::eWH_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4836 of file NPSMEFTd6.h.

◆ eWH_2_HD

double NPSMEFTd6::eWH_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4838 of file NPSMEFTd6.h.

◆ eWH_2_HQ3_11

double NPSMEFTd6::eWH_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4837 of file NPSMEFTd6.h.

◆ eWH_2_HW

double NPSMEFTd6::eWH_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4839 of file NPSMEFTd6.h.

◆ eWH_2_HWB

double NPSMEFTd6::eWH_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV).

Definition at line 4840 of file NPSMEFTd6.h.

◆ eWH_78_DeltaGF

double NPSMEFTd6::eWH_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 4850 of file NPSMEFTd6.h.

◆ eWH_78_DHW

double NPSMEFTd6::eWH_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV).

Definition at line 4849 of file NPSMEFTd6.h.

◆ eWH_78_Hbox

double NPSMEFTd6::eWH_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4844 of file NPSMEFTd6.h.

◆ eWH_78_HD

double NPSMEFTd6::eWH_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4846 of file NPSMEFTd6.h.

◆ eWH_78_HQ3_11

double NPSMEFTd6::eWH_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4845 of file NPSMEFTd6.h.

◆ eWH_78_HW

double NPSMEFTd6::eWH_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4847 of file NPSMEFTd6.h.

◆ eWH_78_HWB

double NPSMEFTd6::eWH_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV).

Definition at line 4848 of file NPSMEFTd6.h.

◆ eWHbb

double NPSMEFTd6::eWHbb
protected

Definition at line 4786 of file NPSMEFTd6.h.

◆ eWHgaga

double NPSMEFTd6::eWHgaga
protected

Definition at line 4786 of file NPSMEFTd6.h.

◆ eWHint

double NPSMEFTd6::eWHint
protected

Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.)

Definition at line 4751 of file NPSMEFTd6.h.

◆ eWHmumu

double NPSMEFTd6::eWHmumu
protected

Total relative theoretical error in \(pp \to WH \to W X\).

Definition at line 4786 of file NPSMEFTd6.h.

◆ eWHpar

double NPSMEFTd6::eWHpar
protected

Parametric relative theoretical error in WH production. (Assumed to be constant in energy.)

Definition at line 4752 of file NPSMEFTd6.h.

◆ eWHtautau

double NPSMEFTd6::eWHtautau
protected

Definition at line 4786 of file NPSMEFTd6.h.

◆ eWHWW

double NPSMEFTd6::eWHWW
protected

Definition at line 4786 of file NPSMEFTd6.h.

◆ eWHZga

double NPSMEFTd6::eWHZga
protected

Definition at line 4786 of file NPSMEFTd6.h.

◆ eWHZZ

double NPSMEFTd6::eWHZZ
protected

Definition at line 4786 of file NPSMEFTd6.h.

◆ eZH_1314_DeltaGF

double NPSMEFTd6::eZH_1314_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4897 of file NPSMEFTd6.h.

◆ eZH_1314_DHB

double NPSMEFTd6::eZH_1314_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4895 of file NPSMEFTd6.h.

◆ eZH_1314_DHW

double NPSMEFTd6::eZH_1314_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4896 of file NPSMEFTd6.h.

◆ eZH_1314_HB

double NPSMEFTd6::eZH_1314_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4892 of file NPSMEFTd6.h.

◆ eZH_1314_Hbox

double NPSMEFTd6::eZH_1314_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4886 of file NPSMEFTd6.h.

◆ eZH_1314_HD

double NPSMEFTd6::eZH_1314_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4891 of file NPSMEFTd6.h.

◆ eZH_1314_Hd_11

double NPSMEFTd6::eZH_1314_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4889 of file NPSMEFTd6.h.

◆ eZH_1314_HQ1_11

double NPSMEFTd6::eZH_1314_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4887 of file NPSMEFTd6.h.

◆ eZH_1314_HQ3_11

double NPSMEFTd6::eZH_1314_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4890 of file NPSMEFTd6.h.

◆ eZH_1314_Hu_11

double NPSMEFTd6::eZH_1314_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4888 of file NPSMEFTd6.h.

◆ eZH_1314_HW

double NPSMEFTd6::eZH_1314_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4893 of file NPSMEFTd6.h.

◆ eZH_1314_HWB

double NPSMEFTd6::eZH_1314_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV).

Definition at line 4894 of file NPSMEFTd6.h.

◆ eZH_2_DeltaGF

double NPSMEFTd6::eZH_2_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4871 of file NPSMEFTd6.h.

◆ eZH_2_DHB

double NPSMEFTd6::eZH_2_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4869 of file NPSMEFTd6.h.

◆ eZH_2_DHW

double NPSMEFTd6::eZH_2_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4870 of file NPSMEFTd6.h.

◆ eZH_2_HB

double NPSMEFTd6::eZH_2_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4866 of file NPSMEFTd6.h.

◆ eZH_2_Hbox

double NPSMEFTd6::eZH_2_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4860 of file NPSMEFTd6.h.

◆ eZH_2_HD

double NPSMEFTd6::eZH_2_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4865 of file NPSMEFTd6.h.

◆ eZH_2_Hd_11

double NPSMEFTd6::eZH_2_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4863 of file NPSMEFTd6.h.

◆ eZH_2_HQ1_11

double NPSMEFTd6::eZH_2_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4861 of file NPSMEFTd6.h.

◆ eZH_2_HQ3_11

double NPSMEFTd6::eZH_2_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4864 of file NPSMEFTd6.h.

◆ eZH_2_Hu_11

double NPSMEFTd6::eZH_2_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4862 of file NPSMEFTd6.h.

◆ eZH_2_HW

double NPSMEFTd6::eZH_2_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4867 of file NPSMEFTd6.h.

◆ eZH_2_HWB

double NPSMEFTd6::eZH_2_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV).

Definition at line 4868 of file NPSMEFTd6.h.

◆ eZH_78_DeltaGF

double NPSMEFTd6::eZH_78_DeltaGF
protected

Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4884 of file NPSMEFTd6.h.

◆ eZH_78_DHB

double NPSMEFTd6::eZH_78_DHB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4882 of file NPSMEFTd6.h.

◆ eZH_78_DHW

double NPSMEFTd6::eZH_78_DHW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4883 of file NPSMEFTd6.h.

◆ eZH_78_HB

double NPSMEFTd6::eZH_78_HB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4879 of file NPSMEFTd6.h.

◆ eZH_78_Hbox

double NPSMEFTd6::eZH_78_Hbox
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4873 of file NPSMEFTd6.h.

◆ eZH_78_HD

double NPSMEFTd6::eZH_78_HD
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4878 of file NPSMEFTd6.h.

◆ eZH_78_Hd_11

double NPSMEFTd6::eZH_78_Hd_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4876 of file NPSMEFTd6.h.

◆ eZH_78_HQ1_11

double NPSMEFTd6::eZH_78_HQ1_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4874 of file NPSMEFTd6.h.

◆ eZH_78_HQ3_11

double NPSMEFTd6::eZH_78_HQ3_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4877 of file NPSMEFTd6.h.

◆ eZH_78_Hu_11

double NPSMEFTd6::eZH_78_Hu_11
protected

Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4875 of file NPSMEFTd6.h.

◆ eZH_78_HW

double NPSMEFTd6::eZH_78_HW
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4880 of file NPSMEFTd6.h.

◆ eZH_78_HWB

double NPSMEFTd6::eZH_78_HWB
protected

Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV).

Definition at line 4881 of file NPSMEFTd6.h.

◆ eZHbb

double NPSMEFTd6::eZHbb
protected

Definition at line 4787 of file NPSMEFTd6.h.

◆ eZHgaga

double NPSMEFTd6::eZHgaga
protected

Definition at line 4787 of file NPSMEFTd6.h.

◆ eZHint

double NPSMEFTd6::eZHint
protected

Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.)

Definition at line 4753 of file NPSMEFTd6.h.

◆ eZHmumu

double NPSMEFTd6::eZHmumu
protected

Total relative theoretical error in \(pp \to ZH \to Z X\).

Definition at line 4787 of file NPSMEFTd6.h.

◆ eZHpar

double NPSMEFTd6::eZHpar
protected

Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.)

Definition at line 4754 of file NPSMEFTd6.h.

◆ eZHtautau

double NPSMEFTd6::eZHtautau
protected

Definition at line 4787 of file NPSMEFTd6.h.

◆ eZHWW

double NPSMEFTd6::eZHWW
protected

Definition at line 4787 of file NPSMEFTd6.h.

◆ eZHZga

double NPSMEFTd6::eZHZga
protected

Definition at line 4787 of file NPSMEFTd6.h.

◆ eZHZZ

double NPSMEFTd6::eZHZZ
protected

Definition at line 4787 of file NPSMEFTd6.h.

◆ FlagFlavU3OfX

bool NPSMEFTd6::FlagFlavU3OfX
private

A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.

Definition at line 5107 of file NPSMEFTd6.h.

◆ FlagHiggsSM

bool NPSMEFTd6::FlagHiggsSM
private

A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables.

Definition at line 5109 of file NPSMEFTd6.h.

◆ FlagLeptonUniversal

const bool NPSMEFTd6::FlagLeptonUniversal
private

An internal boolean flag that is true if assuming lepton flavour universality.

Definition at line 5117 of file NPSMEFTd6.h.

◆ FlagLoopH3d6Quad

bool NPSMEFTd6::FlagLoopH3d6Quad
private

A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling.

Definition at line 5111 of file NPSMEFTd6.h.

◆ FlagLoopHd6

bool NPSMEFTd6::FlagLoopHd6
private

A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions.

Definition at line 5110 of file NPSMEFTd6.h.

◆ FlagPartialQFU

bool NPSMEFTd6::FlagPartialQFU
private

A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators.

Definition at line 5106 of file NPSMEFTd6.h.

◆ FlagQuadraticTerms

bool NPSMEFTd6::FlagQuadraticTerms
private

A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.

Definition at line 5104 of file NPSMEFTd6.h.

◆ FlagQuarkUniversal

const bool NPSMEFTd6::FlagQuarkUniversal
private

An internal boolean flag that is true if assuming quark flavour universality.

Definition at line 5123 of file NPSMEFTd6.h.

◆ FlagRotateCHWCHB

bool NPSMEFTd6::FlagRotateCHWCHB
private

A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB.

Definition at line 5105 of file NPSMEFTd6.h.

◆ FlagUnivOfX

bool NPSMEFTd6::FlagUnivOfX
private

A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively).

Definition at line 5108 of file NPSMEFTd6.h.

◆ g1_tree

double NPSMEFTd6::g1_tree
protected

The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole).

Definition at line 5003 of file NPSMEFTd6.h.

◆ g2_tree

double NPSMEFTd6::g2_tree
protected

The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole).

Definition at line 5004 of file NPSMEFTd6.h.

◆ g3_tree

double NPSMEFTd6::g3_tree
protected

The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole).

Definition at line 5005 of file NPSMEFTd6.h.

◆ GammaHTotR

double NPSMEFTd6::GammaHTotR
protected

NP contributions and Total to Higgs width ratio with SM.

Definition at line 5042 of file NPSMEFTd6.h.

◆ gZdL

double NPSMEFTd6::gZdL
protected

Definition at line 5010 of file NPSMEFTd6.h.

◆ gZdR

double NPSMEFTd6::gZdR
protected

The tree level value of the \(Z\bar{d}d\) couplings in the SM.

Definition at line 5010 of file NPSMEFTd6.h.

◆ gZlL

double NPSMEFTd6::gZlL
protected

Definition at line 5008 of file NPSMEFTd6.h.

◆ gZlR

double NPSMEFTd6::gZlR
protected

The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM.

Definition at line 5008 of file NPSMEFTd6.h.

◆ gZuL

double NPSMEFTd6::gZuL
protected

Definition at line 5009 of file NPSMEFTd6.h.

◆ gZuR

double NPSMEFTd6::gZuR
protected

The tree level value of the \(Z\bar{u}u\) couplings in the SM.

Definition at line 5009 of file NPSMEFTd6.h.

◆ gZvL

double NPSMEFTd6::gZvL
protected

The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM.

Definition at line 5007 of file NPSMEFTd6.h.

◆ Lambda_NP

double NPSMEFTd6::Lambda_NP
protected

The new physics scale [GeV].

Definition at line 4743 of file NPSMEFTd6.h.

◆ lambdaH_tree

double NPSMEFTd6::lambdaH_tree
protected

The SM tree level value of the scalar quartic coupling in the potential.

Definition at line 5020 of file NPSMEFTd6.h.

◆ LambdaNP2

double NPSMEFTd6::LambdaNP2
protected

The square of the new physics scale [GeV \(^2\)].

Definition at line 4925 of file NPSMEFTd6.h.

◆ lambZ

double NPSMEFTd6::lambZ
protected

Independent contribution to aTGC.

Definition at line 4919 of file NPSMEFTd6.h.

◆ NNPSMEFTd6Vars

const int NPSMEFTd6::NNPSMEFTd6Vars = 506
static

The number of the model parameters in NPSMEFTd6.

 

Definition at line 891 of file NPSMEFTd6.h.

◆ NNPSMEFTd6Vars_LFU_QFU

const int NPSMEFTd6::NNPSMEFTd6Vars_LFU_QFU = 260
static

The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.

 

Definition at line 909 of file NPSMEFTd6.h.

◆ NPSMEFTd6M

Matching<NPSMEFTd6Matching,NPSMEFTd6> NPSMEFTd6::NPSMEFTd6M
mutableprotected

Definition at line 4471 of file NPSMEFTd6.h.

◆ NPSMEFTd6Vars

const std::string NPSMEFTd6::NPSMEFTd6Vars
static

A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false.

Definition at line 897 of file NPSMEFTd6.h.

◆ NPSMEFTd6Vars_LFU_QFU

const std::string NPSMEFTd6::NPSMEFTd6Vars_LFU_QFU
static

A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false.

Definition at line 916 of file NPSMEFTd6.h.

◆ NPSMEFTd6VarsRot

const std::string NPSMEFTd6::NPSMEFTd6VarsRot
static

A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true.

Definition at line 903 of file NPSMEFTd6.h.

◆ NPSMEFTd6VarsRot_LFU_QFU

const std::string NPSMEFTd6::NPSMEFTd6VarsRot_LFU_QFU
static

A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true.

Definition at line 923 of file NPSMEFTd6.h.

◆ sW2_tree

double NPSMEFTd6::sW2_tree
protected

The square of the tree level values for the sine of the weak angle.

Definition at line 5001 of file NPSMEFTd6.h.

◆ sW_tree

double NPSMEFTd6::sW_tree
protected

The tree level values for the sine of the weak angle.

Definition at line 4999 of file NPSMEFTd6.h.

◆ UevL

double NPSMEFTd6::UevL
protected

The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.)

Definition at line 5012 of file NPSMEFTd6.h.

◆ v2

double NPSMEFTd6::v2
protected

The square of the EW vev.

Definition at line 4993 of file NPSMEFTd6.h.

◆ v2_over_LambdaNP2

double NPSMEFTd6::v2_over_LambdaNP2
protected

The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).

Definition at line 4994 of file NPSMEFTd6.h.

◆ VudL

double NPSMEFTd6::VudL
protected

The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.)

Definition at line 5013 of file NPSMEFTd6.h.

◆ w_WW

gsl_integration_cquad_workspace* NPSMEFTd6::w_WW
private

Gsl integral variable

Definition at line 5125 of file NPSMEFTd6.h.

◆ Yukb

double NPSMEFTd6::Yukb
protected

SM d-quark Yukawas.

Definition at line 5032 of file NPSMEFTd6.h.

◆ Yukc

double NPSMEFTd6::Yukc
protected

Definition at line 5031 of file NPSMEFTd6.h.

◆ Yukd

double NPSMEFTd6::Yukd
protected

Definition at line 5032 of file NPSMEFTd6.h.

◆ Yuke

double NPSMEFTd6::Yuke
protected

Definition at line 5030 of file NPSMEFTd6.h.

◆ Yukmu

double NPSMEFTd6::Yukmu
protected

Definition at line 5030 of file NPSMEFTd6.h.

◆ Yuks

double NPSMEFTd6::Yuks
protected

Definition at line 5032 of file NPSMEFTd6.h.

◆ Yukt

double NPSMEFTd6::Yukt
protected

SM u-quark Yukawas.

Definition at line 5031 of file NPSMEFTd6.h.

◆ Yuktau

double NPSMEFTd6::Yuktau
protected

SM lepton Yukawas.

Definition at line 5030 of file NPSMEFTd6.h.

◆ Yuku

double NPSMEFTd6::Yuku
protected

Definition at line 5031 of file NPSMEFTd6.h.


The documentation for this class was generated from the following files:
QCD::TAU
Definition: QCD.h:316
NPSMEFTd6::CHud_12i
double CHud_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4563
NPSMEFTd6::deltaMwd6
virtual double deltaMwd6() const
The relative NP corrections to the mass of the boson, .
Definition: NPSMEFTd6.cpp:3075
NPSMEFTd6::eggFHZZ
double eggFHZZ
Definition: NPSMEFTd6.h:4784
NPSMEFTd6::CuB_23r
double CuB_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4632
NPSMEFTd6::CHud_33r
double CHud_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4561
NPSMEFTd6::CeB_11r
double CeB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4688
sigmattH
Definition: NPSMEFT6dtopquark.h:659
NPSMEFTd6::lambZ
double lambZ
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:4919
NPSMEFTd6::deltaGammaTotalRatio1noError
virtual double deltaGammaTotalRatio1noError() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10931
NPSMEFTd6::CpLedQ_11
double CpLedQ_11
Definition: NPSMEFTd6.h:4742
NPSMEFTd6::CdG_12i
double CdG_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4647
NPSMEFTd6::C2BS
double C2BS
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4477
NPSMEFTd6::delta_ZZ
double delta_ZZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:5015
gslpp::cos
complex cos(const complex &z)
Definition: gslpp_complex.cpp:429
NPSMEFTd6::Yuku
double Yuku
Definition: NPSMEFTd6.h:5031
NPSMEFTd6::eggFHtautau
double eggFHtautau
Definition: NPSMEFTd6.h:4784
NPSMEFTd6::CdW_13r
double CdW_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4654
NPSMEFTd6::g3_tree
double g3_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:5005
NPSMEFTd6::CLQ1_3113
double CLQ1_3113
Definition: NPSMEFTd6.h:4705
NPSMEFTd6::CLu_2211
double CLu_2211
Definition: NPSMEFTd6.h:4729
QCD::NEUTRINO_3
Definition: QCD.h:315
NPSMEFTd6::CeW_12r
double CeW_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4677
NPSMEFTd6::CLQ3_3113
double CLQ3_3113
Definition: NPSMEFTd6.h:4710
NPSMEFTd6::GammaHmumuRatio
double GammaHmumuRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12477
NPSMEFTd6::CHL1_23i
double CHL1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4501
NPSMEFTd6::CLd_2211
double CLd_2211
Definition: NPSMEFTd6.h:4733
NPSMEFTd6::deltag1ZNP
virtual double deltag1ZNP() const
The new physics contribution to the anomalous triple gauge coupling .
Definition: NPSMEFTd6.cpp:13819
NPSMEFTd6::obliqueS
virtual double obliqueS() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2927
NPSMEFTd6::dxseeWWdcosBin
virtual double dxseeWWdcosBin(const double sqrt_s, const double cos1, const double cos2) const
The integral of differential distribution for , with in a given bin of the polar angle.
Definition: NPSMEFTd6.cpp:14188
NPSMEFTd6::ettH_78_uG_33r
double ettH_78_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4906
StandardModel::cW2
virtual double cW2(const double Mw_i) const
The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as .
Definition: StandardModel.cpp:1015
NPSMEFTd6::CHud_11r
double CHud_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4556
NPSMEFTd6::CiH
double CiH
Definition: NPSMEFTd6.h:4964
NPSMEFTd6::eWH_1314_HW
double eWH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4855
NPSMEFTd6::eVBF_1314_DeltaGF
double eVBF_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4834
NPSMEFTd6::eHWWpar
double eHWWpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4768
StandardModel::setParameter
virtual void setParameter(const std::string name, const double &value)
A method to set the value of a parameter of StandardModel.
Definition: StandardModel.cpp:257
NPSMEFTd6::CdG_12r
double CdG_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4641
NPSMEFTd6::deltaGammaHZeeRatio2
double deltaGammaHZeeRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11599
StandardModel::v
virtual double v() const
The Higgs vacuum expectation value.
Definition: StandardModel.cpp:943
NPSMEFTd6::GammaW
virtual double GammaW() const
The total width of the boson, .
Definition: NPSMEFTd6.cpp:3137
NPSMEFTd6::ettHbb
double ettHbb
Definition: NPSMEFTd6.h:4788
NPSMEFTd6::gZlL
double gZlL
Definition: NPSMEFTd6.h:5008
NPSMEFTd6::CHd_23r
double CHd_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4551
NPSMEFTd6::Yukmu
double Yukmu
Definition: NPSMEFTd6.h:5030
NPSMEFTd6::deltaGammaHZuuRatio2
double deltaGammaHZuuRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12098
NPSMEFTd6::CeH_11r
double CeH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4568
NPSMEFTd6::aiT
double aiT
Definition: NPSMEFTd6.h:5036
NPSMEFTd6::CQe_2333
double CQe_2333
Definition: NPSMEFTd6.h:4740
NPSMEFTd6::cW2_tree
double cW2_tree
The square of the tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:5000
NPSMEFTd6::CHQ1_33
double CHQ1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4525
NPSMEFTd6::deltaGammaHZmumuRatio2
double deltaGammaHZmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11660
NPSMEFTd6::eHggpar
double eHggpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4766
NPSMEFTd6::obliqueT
virtual double obliqueT() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2932
QCD::BOTTOM
Definition: QCD.h:329
NPSMEFTd6::CLd_1132
double CLd_1132
Definition: NPSMEFTd6.h:4736
NPSMEFTd6::eZH_2_Hd_11
double eZH_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4863
NPSMEFTd6::deltaGammaHmumuRatio1
double deltaGammaHmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12493
NPSMEFTd6::CiHd_33
double CiHd_33
Definition: NPSMEFTd6.h:4952
NPSMEFTd6::deltaGammaHZZ4muRatio2
double deltaGammaHZZ4muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11918
NPSMEFTd6::eZHbb
double eZHbb
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::NNPSMEFTd6Vars
static const int NNPSMEFTd6Vars
The number of the model parameters in NPSMEFTd6.
Definition: NPSMEFTd6.h:891
NPSMEFTd6::gZlR
double gZlR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:5008
NPSMEFTd6::Ceu_1111
double Ceu_1111
Definition: NPSMEFTd6.h:4716
NPSMEFTd6::BrHZZ4muRatio
virtual double BrHZZ4muRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10491
NPSMEFTd6::CuW_13r
double CuW_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4618
NPSMEFTd6::cgg_HB
virtual double cgg_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15580
NPSMEFTd6::CeH_23r
double CeH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4572
NPSMEFTd6::CLd_2223
double CLd_2223
Definition: NPSMEFTd6.h:4735
NPSMEFTd6::CLQ1_1331
double CLQ1_1331
Definition: NPSMEFTd6.h:4705
NPSMEFTd6::CLQ1_2211
double CLQ1_2211
Definition: NPSMEFTd6.h:4704
NPSMEFTd6::CuG_12i
double CuG_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4611
Particle::is
bool is(std::string name_i) const
Definition: Particle.cpp:23
NPSMEFTd6::deltaGammaHbbRatio2
double deltaGammaHbbRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12703
NPSMEFTd6::ettH_1314_G
double ettH_1314_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4910
StandardModel::computeSigmaWH
double computeSigmaWH(const double sqrt_s) const
The WH production cross section in the Standard Model.
Definition: StandardModel.h:2102
NPSMEFTd6::CLQ1_2232
double CLQ1_2232
Definition: NPSMEFTd6.h:4707
NPSMEFTd6::CiHB
double CiHB
Definition: NPSMEFTd6.h:4957
NPSMEFTd6::deltaGammaHZgaRatio1
double deltaGammaHZgaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12332
NPSMEFTd6::eWH_78_HQ3_11
double eWH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4845
StandardModel::gamma
double gamma
used as an input for FlagWolfenstein = FALSE
Definition: StandardModel.h:2575
NPSMEFTd6::CLQ3_1133
double CLQ3_1133
Definition: NPSMEFTd6.h:4710
NPSMEFTd6::eHggint
double eHggint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4765
NPSMEFTd6::CLQ1_1123
double CLQ1_1123
Definition: NPSMEFTd6.h:4706
NPSMEFTd6::eZHmumu
double eZHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::ettH_1314_DeltagHt
double ettH_1314_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4912
NPSMEFTd6::C2W
double C2W
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4476
NPSMEFTd6::eWH_2_Hbox
double eWH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4836
NPSMEFTd6::eZH_1314_HB
double eZH_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4892
NPSMEFTd6::CLd_1111
double CLd_1111
Definition: NPSMEFTd6.h:4732
NPSMEFTd6::CidH_22r
double CidH_22r
Definition: NPSMEFTd6.h:4975
gslpp::matrix< double >
A class for constructing and defining operations on real matrices.
Definition: gslpp_matrix_double.h:48
NPSMEFTd6::CHd_11
double CHd_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4547
NPSMEFTd6::CLd_3332
double CLd_3332
Definition: NPSMEFTd6.h:4736
NPSMEFTd6::CHe_23i
double CHe_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4519
NPSMEFTd6::deltayc_HB
virtual double deltayc_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15502
NPSMEFTd6::FlagHiggsSM
bool FlagHiggsSM
A boolean flag that is true if including dependence on small variations of the SM parameters (depende...
Definition: NPSMEFTd6.h:5109
NPSMEFTd6::CiLL_2112
double CiLL_2112
Definition: NPSMEFTd6.h:4991
NPSMEFTd6::CLe_2211
double CLe_2211
Definition: NPSMEFTd6.h:4726
NPSMEFTd6::muVH
virtual double muVH(const double sqrt_s) const
The ratio between the WH+ZH associated production cross-section in the current model and in the Stan...
Definition: NPSMEFTd6.cpp:9050
NPSMEFTd6::CHf_diag
double CHf_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPSMEFTd6.cpp:2774
NPSMEFTd6::CHud_33i
double CHud_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4567
NPSMEFTd6::CidH_33r
double CidH_33r
Definition: NPSMEFTd6.h:4976
NPSMEFTd6::CdH_22r
double CdH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4595
NPSMEFTd6::CLedQ_22
double CLedQ_22
Definition: NPSMEFTd6.h:4742
NPSMEFTd6::CHud_13r
double CHud_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4558
NPSMEFTd6::BrHtautauRatio
virtual double BrHtautauRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10814
NPSMEFTd6::eHZgapar
double eHZgapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4772
NPSMEFTd6Matching::updateNPSMEFTd6Parameters
void updateNPSMEFTd6Parameters()
Updates to new FlavourWilsonCoefficient parameter sets.
Definition: NPSMEFTd6Matching.cpp:24
NPSMEFTd6::eWHWW
double eWHWW
Definition: NPSMEFTd6.h:4786
NPSMEFTd6::CHu_12i
double CHu_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4544
NPSMEFTd6::CiHQ1_22
double CiHQ1_22
Definition: NPSMEFTd6.h:4936
NPSMEFTd6::CHL3_12i
double CHL3_12i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4508
NPSMEFTd6::eepZBFint
double eepZBFint
Intrinsic relative theoretical error in via ZBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4763
StandardModel::computeBrHtotautau
double computeBrHtotautau() const
The Br in the Standard Model.
Definition: StandardModel.h:2278
NPSMEFTd6::CHu_13r
double CHu_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4540
NPSMEFTd6::CQe_3222
double CQe_3222
Definition: NPSMEFTd6.h:4741
NPSMEFTd6::BrHgagaRatio
virtual double BrHgagaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10762
NPSMEFTd6::CHQ1_13i
double CHQ1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4527
NPSMEFTd6::aleMz
double aleMz
The em constant at Mz.
Definition: NPSMEFTd6.h:4995
NPSMEFTd6::deltamtau
virtual double deltamtau() const
The relative correction to the mass of the lepton, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:3009
NPSMEFTd6::eZHint
double eZHint
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4753
NPSMEFTd6::eZH_2_HW
double eZH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4867
NPSMEFTd6::CeB_23r
double CeB_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4692
NPSMEFTd6::CHe_23r
double CHe_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4515
NPSMEFTd6::CLQ3_2211
double CLQ3_2211
Definition: NPSMEFTd6.h:4709
NPSMEFTd6::deltaGammaHZmumuRatio1
double deltaGammaHZmumuRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11625
NPSMEFTd6::deltaGammaHZZ4vRatio2
double deltaGammaHZZ4vRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12039
NPSMEFTd6::CHQ1_23i
double CHQ1_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4528
NPSMEFTd6::CuB_22r
double CuB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4631
NPSMEFTd6::ettH_2_DeltagHt
double ettH_2_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4902
NPSMEFTd6::Ceu_2211
double Ceu_2211
Definition: NPSMEFTd6.h:4717
NPSMEFTd6::CLL_1122
double CLL_1122
Definition: NPSMEFTd6.h:4701
NPSMEFTd6::deltaGammaHWW4fRatio2
double deltaGammaHWW4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11431
NPSMEFTd6::Ceu_1133
double Ceu_1133
Definition: NPSMEFTd6.h:4718
NPSMEFTd6::Ceu_3311
double Ceu_3311
Definition: NPSMEFTd6.h:4718
NPSMEFTd6::CuG_23i
double CuG_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4614
NPSMEFTd6::aiHQ
double aiHQ
Definition: NPSMEFTd6.h:5038
NPSMEFTd6::CdH_13i
double CdH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4600
NPSMEFTd6::g1_tree
double g1_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:5003
NPSMEFTd6::CQe_3211
double CQe_3211
Definition: NPSMEFTd6.h:4741
NPSMEFTd6::BrHbbRatio
virtual double BrHbbRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10866
NPSMEFTd6::CHQ3_22
double CHQ3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4532
NPSMEFTd6::FlagLoopHd6
bool FlagLoopHd6
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to th...
Definition: NPSMEFTd6.h:5110
NPSMEFTd6::Yukt
double Yukt
SM u-quark Yukawas.
Definition: NPSMEFTd6.h:5031
NPSMEFTd6::eHgagapar
double eHgagapar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4774
NPSMEFTd6::GammaHTotR
double GammaHTotR
NP contributions and Total to Higgs width ratio with SM.
Definition: NPSMEFTd6.h:5042
NPbase::NPbase
NPbase()
The default constructor.
Definition: NPbase.cpp:10
NPSMEFTd6::CHL1_13r
double CHL1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4495
NPSMEFTd6::eHccint
double eHccint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4779
NPSMEFTd6::eVHinv
double eVHinv
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4789
NPSMEFTd6::eggFHgaga
double eggFHgaga
Definition: NPSMEFTd6.h:4784
NPSMEFTd6::CLQ3_1331
double CLQ3_1331
Definition: NPSMEFTd6.h:4710
NPSMEFTd6::deltayb_HB
virtual double deltayb_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15480
NPSMEFTd6::aiA
double aiA
Definition: NPSMEFTd6.h:5037
NPSMEFTd6::CHL1_33
double CHL1_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4498
NPSMEFTd6::CHu_13i
double CHu_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4545
NPSMEFTd6::Mw
virtual double Mw() const
The mass of the boson, .
Definition: NPSMEFTd6.cpp:3067
NPSMEFTd6::CHd_13r
double CHd_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4549
gslpp::sin
complex sin(const complex &z)
Definition: gslpp_complex.cpp:420
NPSMEFTd6::Ced_2211
double Ced_2211
Definition: NPSMEFTd6.h:4721
NPSMEFTd6::eWHZZ
double eWHZZ
Definition: NPSMEFTd6.h:4786
NPSMEFTd6::deltaGammaHZZ4eRatio1
double deltaGammaHZZ4eRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11756
Matching::getObj
T & getObj()
Definition: Matching.h:14
NPSMEFTd6::CLd_3323
double CLd_3323
Definition: NPSMEFTd6.h:4735
NPbase::BR_Zf
virtual double BR_Zf(const Particle f) const
The Branching ratio of the boson into a given fermion pair, .
Definition: NPbase.cpp:262
NPSMEFTd6::eepWBFpar
double eepWBFpar
Parametric relative theoretical error in via WBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4762
NPSMEFTd6::CLd_1122
double CLd_1122
Definition: NPSMEFTd6.h:4733
NPSMEFTd6::LambdaNP2
double LambdaNP2
The square of the new physics scale [GeV ].
Definition: NPSMEFTd6.h:4925
NPSMEFTd6::deltamc
virtual double deltamc() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2998
NPSMEFTd6::CLedQ_11
double CLedQ_11
Definition: NPSMEFTd6.h:4742
NPSMEFTd6::FlagLoopH3d6Quad
bool FlagLoopH3d6Quad
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables...
Definition: NPSMEFTd6.h:5111
NPSMEFTd6::deltaGammaHccRatio1
double deltaGammaHccRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12598
NPSMEFTd6::deltaGammaHZgaRatio2
double deltaGammaHZgaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12391
NPSMEFTd6::Ced_3311
double Ced_3311
Definition: NPSMEFTd6.h:4722
NPSMEFTd6::CdW_23i
double CdW_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4662
NPSMEFTd6::CLu_2233
double CLu_2233
Definition: NPSMEFTd6.h:4731
NPSMEFTd6::dKappaga
double dKappaga
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:4918
NPSMEFTd6::deltaGammaHWW4fRatio1
double deltaGammaHWW4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11387
NPSMEFTd6::CuW_11i
double CuW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4622
NPSMEFTd6::CLu_3311
double CLu_3311
Definition: NPSMEFTd6.h:4730
NPSMEFTd6::CdG_13r
double CdG_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4642
QCD::UP
Definition: QCD.h:324
NPSMEFTd6::CieH_11r
double CieH_11r
Definition: NPSMEFTd6.h:4966
NPSMEFTd6::eZH_1314_Hu_11
double eZH_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4888
StandardModel::GF
double GF
The Fermi constant in .
Definition: StandardModel.h:2555
NPSMEFTd6::CLQ1_2223
double CLQ1_2223
Definition: NPSMEFTd6.h:4706
NPSMEFTd6::deltaGammaHZvvRatio1
double deltaGammaHZvvRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11944
NPSMEFTd6::eVBF_1314_Hbox
double eVBF_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4822
NPSMEFTd6::CHud_diag
gslpp::complex CHud_diag(const Particle u) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPSMEFTd6.cpp:2800
NPSMEFTd6::Ced_3332
double Ced_3332
Definition: NPSMEFTd6.h:4724
NPSMEFTd6::CHe_33
double CHe_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4516
NPSMEFTd6::FlagPartialQFU
bool FlagPartialQFU
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd fa...
Definition: NPSMEFTd6.h:5106
NPSMEFTd6::CiuW_33r
double CiuW_33r
Definition: NPSMEFTd6.h:4984
Model::addMissingModelParameter
void addMissingModelParameter(const std::string &missingParameterName)
Definition: Model.h:240
NPSMEFTd6::CdG_22r
double CdG_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4643
NPSMEFTd6::CHd_12r
double CHd_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4548
NPSMEFTd6::eVBFHgaga
double eVBFHgaga
Definition: NPSMEFTd6.h:4785
NPSMEFTd6::CHW
double CHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4480
StandardModel::CheckParameters
virtual bool CheckParameters(const std::map< std::string, double > &DPars)
A method to check if all the mandatory parameters for StandardModel have been provided in model initi...
Definition: StandardModel.cpp:339
NPSMEFTd6::CDHW
double CDHW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4485
NPSMEFTd6::muZH
virtual double muZH(const double sqrt_s) const
The ratio between the Z-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:7357
NPSMEFTd6::CHud_22i
double CHud_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4565
StandardModel::alphaMz
double alphaMz() const
The electromagnetic coupling at the -mass scale, .
Definition: StandardModel.cpp:893
NPSMEFTd6::deltaG_hhhRatio
virtual double deltaG_hhhRatio() const
The new physics contribution to the Higgs self-coupling . Normalized to the SM value.
Definition: NPSMEFTd6.cpp:3458
NPSMEFTd6::CLQ3_1132
double CLQ3_1132
Definition: NPSMEFTd6.h:4712
NPSMEFTd6::NPSMEFTd6Vars_LFU_QFU
static const std::string NPSMEFTd6Vars_LFU_QFU[NNPSMEFTd6Vars_LFU_QFU]
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavo...
Definition: NPSMEFTd6.h:916
NPSMEFTd6::CQe_3233
double CQe_3233
Definition: NPSMEFTd6.h:4741
NPSMEFTd6::deltaG_hff
virtual gslpp::complex deltaG_hff(const Particle p) const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:3444
NPSMEFTd6::CiuB_33r
double CiuB_33r
Definition: NPSMEFTd6.h:4988
NPSMEFTd6::deltaGzd6
virtual double deltaGzd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:3154
NPSMEFTd6::BrHinv
double BrHinv
The branching ratio of invisible Higgs decays.
Definition: NPSMEFTd6.h:4914
QCD::CHARM
Definition: QCD.h:326
NPSMEFTd6::CdG_11r
double CdG_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4640
NPSMEFTd6::cZBox_HB
virtual double cZBox_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15534
NPSMEFTd6::aiHB
double aiHB
Definition: NPSMEFTd6.h:5036
NPSMEFTd6::ai3G
double ai3G
Definition: NPSMEFTd6.h:5035
NPSMEFTd6::CQe_1122
double CQe_1122
Definition: NPSMEFTd6.h:4738
NPSMEFTd6::aipHQ
double aipHQ
Definition: NPSMEFTd6.h:5038
NPSMEFTd6::cW_tree
double cW_tree
The tree level values for the cosine of the weak angle.
Definition: NPSMEFTd6.h:4998
NPbase::deltaGamma_Z
virtual double deltaGamma_Z() const
The new physics contribution to the total decay width of the boson, .
Definition: NPbase.cpp:176
NPSMEFTd6::deltaGammaHZeeRatio1
double deltaGammaHZeeRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11564
NPSMEFTd6::CLQ1_1122
double CLQ1_1122
Definition: NPSMEFTd6.h:4704
StandardModel::computeBrHtobb
double computeBrHtobb() const
The Br in the Standard Model.
Definition: StandardModel.h:2313
NPSMEFTd6::eZHZZ
double eZHZZ
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::eVBF_2_HWB
double eVBF_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4802
NPSMEFTd6::deltaG1_hZA
virtual double deltaG1_hZA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:3296
NPSMEFTd6::eZH_78_HQ3_11
double eZH_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4877
NPSMEFTd6::deltaGammaHZffRatio1
double deltaGammaHZffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:12183
NPSMEFTd6::eVBF_1314_HD
double eVBF_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4827
NPSMEFTd6::CeB_12i
double CeB_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4695
NPSMEFTd6::CuB_13r
double CuB_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4630
NPSMEFTd6::eZH_78_HD
double eZH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4878
NPSMEFTd6::CdB_11i
double CdB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4670
NPSMEFTd6::CHQ3_12i
double CHQ3_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4535
gslpp::complex
A class for defining operations on and functions of complex numbers.
Definition: gslpp_complex.h:35
Matching::setObj
void setObj(T &obji)
Definition: Matching.h:15
NPSMEFTd6::BrHexo
double BrHexo
The branching ratio of exotic (not invisible) Higgs decays.
Definition: NPSMEFTd6.h:4915
NPSMEFTd6::deltaa0
virtual double deltaa0() const
The relative correction to the electromagnetic constant at zero momentum, , with respect to ref....
Definition: NPSMEFTd6.cpp:3042
NPSMEFTd6::deltaGammaHZuuRatio1
double deltaGammaHZuuRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12065
StandardModel::mHl
double mHl
The Higgs mass in GeV.
Definition: StandardModel.h:2558
NPSMEFTd6::deltaGammaHZZ4muRatio1
double deltaGammaHZZ4muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11881
NPSMEFTd6::CdW_33r
double CdW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4657
NPSMEFTd6::eggFHWW
double eggFHWW
Definition: NPSMEFTd6.h:4784
QCD::NEUTRINO_2
Definition: QCD.h:313
NPSMEFTd6::dZH
double dZH
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition: NPSMEFTd6.h:5022
NPSMEFTd6::eWH_2_HWB
double eWH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4840
gslpp::log
complex log(const complex &z)
Definition: gslpp_complex.cpp:342
NPSMEFTd6::CLQ3_3332
double CLQ3_3332
Definition: NPSMEFTd6.h:4712
NPSMEFTd6::eZHgaga
double eZHgaga
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::CiuW_11r
double CiuW_11r
Definition: NPSMEFTd6.h:4982
NPSMEFTd6::CeB_11i
double CeB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4694
NPSMEFTd6::v2
double v2
The square of the EW vev.
Definition: NPSMEFTd6.h:4993
NPSMEFTd6::ettH_78_DeltagHt
double ettH_78_DeltagHt
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4907
NPSMEFTd6::v2_over_LambdaNP2
double v2_over_LambdaNP2
The ratio between the EW vev and the new physics scale, squared .
Definition: NPSMEFTd6.h:4994
NPSMEFTd6::CLu_1111
double CLu_1111
Definition: NPSMEFTd6.h:4728
gslpp::matrix< gslpp::complex >
NPSMEFTd6::CuG_23r
double CuG_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4608
NPSMEFTd6::NPSMEFTd6VarsRot_LFU_QFU
static const std::string NPSMEFTd6VarsRot_LFU_QFU[NNPSMEFTd6Vars_LFU_QFU]
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavo...
Definition: NPSMEFTd6.h:923
NPSMEFTd6::CHL1_23r
double CHL1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4497
NPSMEFTd6::CeH_12i
double CeH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4575
NPSMEFTd6::CLQ3_3311
double CLQ3_3311
Definition: NPSMEFTd6.h:4710
NPSMEFTd6::CieH_22r
double CieH_22r
Definition: NPSMEFTd6.h:4967
NPSMEFTd6::CuG_12r
double CuG_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4605
NPSMEFTd6::gZdL
double gZdL
Definition: NPSMEFTd6.h:5010
NPSMEFTd6::CLd_2232
double CLd_2232
Definition: NPSMEFTd6.h:4736
NPSMEFTd6::eZHtautau
double eZHtautau
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::deltaMh
virtual double deltaMh() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2965
NPSMEFTd6::ettH_1314_HG
double ettH_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4909
NPSMEFTd6::CeH_33r
double CeH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4573
NPSMEFTd6::CiHW
double CiHW
Definition: NPSMEFTd6.h:4956
NPSMEFTd6::CeH_13i
double CeH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4576
QCD::ELECTRON
Definition: QCD.h:312
NPSMEFTd6::eWH_1314_HD
double eWH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4854
cgagaHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:2996
Particle::getIsospin
double getIsospin() const
A get method to access the particle isospin.
Definition: Particle.h:115
NPSMEFTd6::CuH_22r
double CuH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4583
NPSMEFTd6::eggFHZga
double eggFHZga
Definition: NPSMEFTd6.h:4784
NPSMEFTd6::FlagLeptonUniversal
const bool FlagLeptonUniversal
An internal boolean flag that is true if assuming lepton flavour universality.
Definition: NPSMEFTd6.h:5117
NPSMEFTd6::deltaGammaHWjjRatio2
double deltaGammaHWjjRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11244
NPSMEFTd6::BrHmumuRatio
virtual double BrHmumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10788
NPSMEFTd6::deltaGammaHZddRatio2
double deltaGammaHZddRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12157
NPSMEFTd6::eZHpar
double eZHpar
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4754
NPSMEFTd6::CidH_11r
double CidH_11r
Definition: NPSMEFTd6.h:4974
gslpp::complex::abs2
double abs2() const
Definition: gslpp_complex.cpp:86
NPSMEFTd6::CHd_13i
double CHd_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4554
NPSMEFTd6::CuB_22i
double CuB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4637
NPSMEFTd6::CuW_33r
double CuW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4621
NPSMEFTd6::eVBF_78_DeltaGF
double eVBF_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4820
NPSMEFTd6::Ced_2223
double Ced_2223
Definition: NPSMEFTd6.h:4723
NPSMEFTd6::deltaG_hAA
virtual double deltaG_hAA() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:3386
NPSMEFTd6::deltamt
virtual double deltamt() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2976
NPSMEFTd6::CHWB
double CHWB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4488
NPSMEFTd6::CHWHB_gaga
double CHWHB_gaga
The combination of dimension-6 operator coefficients entering in : .
Definition: NPSMEFTd6.h:4482
NPSMEFTd6::CiuB_11r
double CiuB_11r
Definition: NPSMEFTd6.h:4986
NPSMEFTd6::eZH_78_Hu_11
double eZH_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4875
NPSMEFTd6::CuH_13i
double CuH_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4588
NPSMEFTd6::CHL1_12i
double CHL1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4499
StandardModel::SMM
Matching< StandardModelMatching, StandardModel > SMM
An object of type Matching.
Definition: StandardModel.h:2550
NPSMEFTd6::eggFHmumu
double eggFHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4784
NPSMEFTd6::mueeZH
virtual double mueeZH(const double sqrt_s) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:7553
NPSMEFTd6::deltaGammaHZZRatio1
double deltaGammaHZZRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11457
NPSMEFTd6::eZH_1314_HW
double eZH_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4893
NPSMEFTd6::CuH_12r
double CuH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4581
NPSMEFTd6::CdW_13i
double CdW_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4660
NPSMEFTd6::CQe_3311
double CQe_3311
Definition: NPSMEFTd6.h:4739
NPSMEFTd6::eZH_2_DHB
double eZH_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4869
NPSMEFTd6::CeB_23i
double CeB_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4698
NPSMEFTd6::CeB_33r
double CeB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4693
cZZHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:2920
NPSMEFTd6::deltaGammaHWW2l2vRatio2
double deltaGammaHWW2l2vRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11188
NPSMEFTd6::CLd_3311
double CLd_3311
Definition: NPSMEFTd6.h:4734
NPSMEFTd6::ettH_78_G
double ettH_78_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4905
NPSMEFTd6::eeMz2
double eeMz2
The em coupling squared (at Mz).
Definition: NPSMEFTd6.h:4997
NPSMEFTd6::CiHQ3_11
double CiHQ3_11
Definition: NPSMEFTd6.h:4938
NPSMEFTd6::eWH_1314_Hbox
double eWH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4852
NPSMEFTd6::eggFHbb
double eggFHbb
Definition: NPSMEFTd6.h:4784
NPSMEFTd6::CHud_23i
double CHud_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4566
NPSMEFTd6::CpLedQ_22
double CpLedQ_22
Definition: NPSMEFTd6.h:4742
NPSMEFTd6::GammaHccRatio
double GammaHccRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12582
NPSMEFTd6::CdG_23i
double CdG_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4650
NPSMEFTd6::eVBFHbb
double eVBFHbb
Definition: NPSMEFTd6.h:4785
NPSMEFTd6::Lambda_NP
double Lambda_NP
The new physics scale [GeV].
Definition: NPSMEFTd6.h:4743
NPSMEFTd6::CiuH_11r
double CiuH_11r
Definition: NPSMEFTd6.h:4970
NPSMEFTd6::Cee_2211
double Cee_2211
Definition: NPSMEFTd6.h:4714
NPSMEFTd6::CLQ1_1132
double CLQ1_1132
Definition: NPSMEFTd6.h:4707
NPSMEFTd6::eVBF_2_HW
double eVBF_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4801
NPSMEFTd6::eZH_78_DeltaGF
double eZH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4884
StandardModel::sW2
virtual double sW2(const double Mw_i) const
The square of the sine of the weak mixing angle in the on-shell scheme, denoted as .
Definition: StandardModel.cpp:1026
NPSMEFTd6::CuW_33i
double CuW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4627
NPSMEFTd6::CiuB_22r
double CiuB_22r
Definition: NPSMEFTd6.h:4987
StandardModel::ale
double ale
The fine-structure constant .
Definition: StandardModel.h:2556
NPSMEFTd6::CHL3_13r
double CHL3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4504
NPSMEFTd6::deltaGammaHWW2l2vRatio1
double deltaGammaHWW2l2vRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11153
NPSMEFTd6::CHu_22
double CHu_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4541
NPSMEFTd6::AH_f
gslpp::complex AH_f(const double tau) const
Fermionic loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:3595
NPSMEFTd6::CdW_22i
double CdW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4661
QCD::mtpole
double mtpole
The pole mass of the top quark.
Definition: QCD.h:927
NPSMEFTd6::CHG
double CHG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4479
NPSMEFTd6::eZH_78_HQ1_11
double eZH_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4874
NPSMEFTd6::deltaGammaHggRatio2
double deltaGammaHggRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11023
NPSMEFTd6::eVBF_2_DHW
double eVBF_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4805
NPSMEFTd6::CeW_12i
double CeW_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4683
NPSMEFTd6::eVBF_1314_HG
double eVBF_1314_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4831
NPSMEFTd6::deltaGammaHWW4jRatio1
double deltaGammaHWW4jRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11270
NPSMEFTd6::CiuH_33r
double CiuH_33r
Definition: NPSMEFTd6.h:4972
StandardModel::setFlag
virtual bool setFlag(const std::string name, const bool value)
A method to set a flag of StandardModel.
Definition: StandardModel.cpp:404
NPSMEFTd6::NPSMEFTd6VarsRot
static const std::string NPSMEFTd6VarsRot[NNPSMEFTd6Vars]
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotat...
Definition: NPSMEFTd6.h:903
NPSMEFTd6::eZH_78_Hbox
double eZH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4873
Model::ModelParamMap
std::map< std::string, std::reference_wrapper< const double > > ModelParamMap
Definition: Model.h:270
NPSMEFTd6::CLQ1_1221
double CLQ1_1221
Definition: NPSMEFTd6.h:4704
NPSMEFTd6::CHe_22
double CHe_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4514
NPSMEFTd6::CLL_1111
double CLL_1111
Definition: NPSMEFTd6.h:4700
NPSMEFTd6::deltaGammaHWffRatio1
double deltaGammaHWffRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11330
NPSMEFTd6::eVBF_1314_DHB
double eVBF_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4832
NPSMEFTd6::CuG_11i
double CuG_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4610
NPSMEFTd6::VudL
double VudL
The tree level value of the couplings in the SM. (Neglecting CKM effects.)
Definition: NPSMEFTd6.h:5013
NPSMEFTd6::eVBF_2_HB
double eVBF_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4800
NPSMEFTd6::CuW_12i
double CuW_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4623
NPSMEFTd6::eVBF_78_HW
double eVBF_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4815
NPSMEFTd6::gZuR
double gZuR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:5009
NPSMEFTd6::g_triangle
gslpp::complex g_triangle(const double tau) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3563
NPSMEFTd6::eVBF_1314_Hd_11
double eVBF_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4825
NPSMEFTd6::CeB_33i
double CeB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4699
NPSMEFTd6::CdG_23r
double CdG_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4644
NPSMEFTd6::GammaHZgaRatio
double GammaHZgaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12316
NPSMEFTd6::FlagQuarkUniversal
const bool FlagQuarkUniversal
An internal boolean flag that is true if assuming quark flavour universality.
Definition: NPSMEFTd6.h:5123
NPSMEFTd6::CHL3_33
double CHL3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4507
NPSMEFTd6::Yukd
double Yukd
Definition: NPSMEFTd6.h:5032
NPSMEFTd6::CHd_33
double CHd_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4552
NPSMEFTd6::eVBF_2_HG
double eVBF_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4803
NPSMEFTd6::ettH_2_uG_33r
double ettH_2_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4901
NPSMEFTd6::eggFint
double eggFint
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4745
NPSMEFTd6::GammaHWWRatio
double GammaHWWRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:11033
NPSMEFTd6::CuW_13i
double CuW_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4624
NPSMEFTd6::eHbbpar
double eHbbpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4782
NPSMEFTd6::ai2G
double ai2G
Definition: NPSMEFTd6.h:5035
NPSMEFTd6::CHQ3_13i
double CHQ3_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4536
NPSMEFTd6::CiHL3_22
double CiHL3_22
Definition: NPSMEFTd6.h:4932
NPSMEFTd6::eHccpar
double eHccpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4780
NPSMEFTd6::eZH_1314_DHB
double eZH_1314_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4895
NPSMEFTd6::CHL1_13i
double CHL1_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4500
NPSMEFTd6::eeMz
double eeMz
The em coupling at Mz.
Definition: NPSMEFTd6.h:4996
NPSMEFTd6::CdW_11r
double CdW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4652
NPSMEFTd6::CiHL1_33
double CiHL1_33
Definition: NPSMEFTd6.h:4930
NPSMEFTd6::deltaGammaHZZ4lRatio1
double deltaGammaHZZ4lRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11686
NPbase::trueSM
StandardModel trueSM
Definition: NPbase.h:2787
NPSMEFTd6::deltaGammaHWlvRatio2
double deltaGammaHWlvRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11127
NPSMEFTd6::eWHint
double eWHint
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4751
StandardModel::computeBrHtoZZ
double computeBrHtoZZ() const
The Br in the Standard Model.
Definition: StandardModel.h:2222
NPSMEFTd6::CHL3_11
double CHL3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4502
NPSMEFTd6::CeB_13i
double CeB_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4696
NPSMEFTd6::eHtautauint
double eHtautauint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4777
NPSMEFTd6::CuH_13r
double CuH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4582
NPSMEFTd6::CLe_1133
double CLe_1133
Definition: NPSMEFTd6.h:4727
NPSMEFTd6::ettHint
double ettHint
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4747
NPSMEFTd6::CHF3_diag
double CHF3_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F.
Definition: NPSMEFTd6.cpp:2756
NPSMEFTd6::I_triangle_2
gslpp::complex I_triangle_2(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3586
NPSMEFTd6::eZH_1314_HWB
double eZH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4894
NPSMEFTd6::cZZ_HB
virtual double cZZ_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15546
NPSMEFTd6::eVBF_78_Hd_11
double eVBF_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4811
NPSMEFTd6::eWH_78_DeltaGF
double eWH_78_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:4850
NPSMEFTd6::CuG_22i
double CuG_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4613
NPSMEFTd6::CiHe_33
double CiHe_33
Definition: NPSMEFTd6.h:4944
NPSMEFTd6::CHQ3_23i
double CHQ3_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4537
StandardModelMatching
A class for the matching in the Standard Model.
Definition: StandardModelMatching.h:26
NPSMEFTd6::GammaHtautauRatio
double GammaHtautauRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12529
NPSMEFTd6::CHu_23i
double CHu_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4546
NPSMEFTd6::CiHL1_22
double CiHL1_22
Definition: NPSMEFTd6.h:4929
NPSMEFTd6::w_WW
gsl_integration_cquad_workspace * w_WW
Definition: NPSMEFTd6.h:5125
NPSMEFTd6::BrHWW2l2vRatio
virtual double BrHWW2l2vRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10260
NPSMEFTd6::CQe_2311
double CQe_2311
Definition: NPSMEFTd6.h:4740
gslpp::complex::conjugate
complex conjugate() const
Definition: gslpp_complex.cpp:288
NPSMEFTd6::eeeWBFint
double eeeWBFint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4755
NPSMEFTd6::deltaaMZ
virtual double deltaaMZ() const
The relative correction to the electromagnetic constant at the Z pole, , with respect to ref....
Definition: NPSMEFTd6.cpp:3031
NPSMEFTd6::deltaGammaHgagaRatio1
double deltaGammaHgagaRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12417
NPSMEFTd6::BrHZZ4lRatio
virtual double BrHZZ4lRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10416
Particle::getMass
const double & getMass() const
A get method to access the particle mass.
Definition: Particle.h:61
NPSMEFTd6::aiWW
double aiWW
Definition: NPSMEFTd6.h:5036
NPSMEFTd6::CdH_13r
double CdH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4594
NPSMEFTd6::CHu_33
double CHu_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4543
NPSMEFTd6::aiuG
double aiuG
Definition: NPSMEFTd6.h:5039
NPSMEFTd6::CiuG_22r
double CiuG_22r
Definition: NPSMEFTd6.h:4979
NPSMEFTd6::eZH_2_DeltaGF
double eZH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4871
NPSMEFTd6::CuG_33r
double CuG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4609
NPSMEFTd6::CeH_22r
double CeH_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4571
NPSMEFTd6::CeH_13r
double CeH_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4570
NPSMEFTd6::CdW_23r
double CdW_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4656
NPSMEFTd6::CLQ1_3332
double CLQ1_3332
Definition: NPSMEFTd6.h:4707
NPSMEFTd6::CuH_22i
double CuH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4589
NPSMEFTd6::deltaGmu
virtual double deltaGmu() const
The relative correction to the muon decay constant, , with respect to ref. point used in the SM calcu...
Definition: NPSMEFTd6.cpp:3020
StandardModel::AlsMz
double AlsMz
The strong coupling constant at the Z-boson mass, .
Definition: StandardModel.h:2553
NPSMEFTd6::CQe_1111
double CQe_1111
Definition: NPSMEFTd6.h:4737
NPSMEFTd6::eZH_1314_Hd_11
double eZH_1314_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4889
NPSMEFTd6::ettHWW
double ettHWW
Definition: NPSMEFTd6.h:4788
NPSMEFTd6::eHmumupar
double eHmumupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4776
NPSMEFTd6::CeW_22i
double CeW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4685
NPSMEFTd6::CHL3_22
double CHL3_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4505
NPSMEFTd6::CiHu_22
double CiHu_22
Definition: NPSMEFTd6.h:4947
NPSMEFTd6::deltacZ_HB
virtual double deltacZ_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15524
NPSMEFTd6::eepWBFint
double eepWBFint
Intrinsic relative theoretical error in via WBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4761
NPSMEFTd6::CiHD
double CiHD
Definition: NPSMEFTd6.h:4963
NPSMEFTd6::deltaKgammaNP
virtual double deltaKgammaNP() const
The new physics contribution to the anomalous triple gauge coupling .
Definition: NPSMEFTd6.cpp:13836
NPSMEFTd6::CuB_33r
double CuB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4633
NPSMEFTd6::ettHgaga
double ettHgaga
Definition: NPSMEFTd6.h:4788
NPSMEFTd6::eWH_1314_DeltaGF
double eWH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4858
NPSMEFTd6::eWHbb
double eWHbb
Definition: NPSMEFTd6.h:4786
NPSMEFTd6::eVBF_1314_HQ3_11
double eVBF_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4826
NPSMEFTd6::CLu_1122
double CLu_1122
Definition: NPSMEFTd6.h:4729
NPSMEFTd6::FlagQuadraticTerms
bool FlagQuadraticTerms
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.
Definition: NPSMEFTd6.h:5104
NPSMEFTd6::CLe_1111
double CLe_1111
Definition: NPSMEFTd6.h:4725
NPSMEFTd6::CuG_13r
double CuG_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4606
NPSMEFTd6::CiHu_11
double CiHu_11
Definition: NPSMEFTd6.h:4946
NPSMEFTd6::eWH_2_DeltaGF
double eWH_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4842
NPSMEFTd6::BrHZddRatio
virtual double BrHZddRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10606
QCD::TOP
Definition: QCD.h:328
NPSMEFTd6::CdH_33i
double CdH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4603
NPSMEFTd6::AH_W
gslpp::complex AH_W(const double tau) const
W loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3600
NPSMEFTd6::BrHZZRatio
virtual double BrHZZRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10386
NPSMEFTd6::eVBF_78_DHB
double eVBF_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4818
NPSMEFTd6::CeW_23r
double CeW_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4680
NPSMEFTd6::CeB_12r
double CeB_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4689
NPSMEFTd6::eZH_1314_HD
double eZH_1314_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4891
NPSMEFTd6::CdH_12r
double CdH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4593
NPSMEFTd6::CdB_33i
double CdB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4675
NPSMEFTd6::deltaGammaHZZ4fRatio1
double deltaGammaHZZ4fRatio1() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:12246
NPSMEFTd6::CLL_1221
double CLL_1221
Definition: NPSMEFTd6.h:4701
gslpp::pow
complex pow(const complex &z1, const complex &z2)
Definition: gslpp_complex.cpp:395
NPSMEFTd6::CLL_3311
double CLL_3311
Definition: NPSMEFTd6.h:4702
NPSMEFTd6::eZH_2_HD
double eZH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4865
NPSMEFTd6::eWHtautau
double eWHtautau
Definition: NPSMEFTd6.h:4786
NPSMEFTd6::cgaga_HB
virtual double cgaga_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15570
NPSMEFTd6::CHe_13i
double CHe_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4518
NPSMEFTd6::eWH_2_HD
double eWH_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4838
NPSMEFTd6::eVBFHinv
double eVBFHinv
Definition: NPSMEFTd6.h:4789
NPSMEFTd6::aiHL
double aiHL
Definition: NPSMEFTd6.h:5038
NPSMEFTd6::eVBF_78_Hbox
double eVBF_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4808
NPSMEFTd6::Ced_1122
double Ced_1122
Definition: NPSMEFTd6.h:4721
Model::raiseMissingModelParameterCount
void raiseMissingModelParameterCount()
Definition: Model.h:250
NPSMEFTd6::mueeWBF
virtual double mueeWBF(const double sqrt_s) const
The ratio between the production cross-section in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:4018
gslpp::sqrt
complex sqrt(const complex &z)
Definition: gslpp_complex.cpp:385
NPSMEFTd6::delta_AZ
double delta_AZ
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:5017
NPSMEFTd6::cHSM
double cHSM
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.
Definition: NPSMEFTd6.h:5024
NPSMEFTd6::BrHWWRatio
virtual double BrHWWRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10228
NPSMEFTd6::eVBF_1314_DHW
double eVBF_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4833
NPSMEFTd6::BrHtoinvRatio
virtual double BrHtoinvRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12794
NPSMEFTd6::eVBF_1314_HB
double eVBF_1314_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4828
NPSMEFTd6::CHQ3_23r
double CHQ3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4533
NPSMEFTd6::CQe_1133
double CQe_1133
Definition: NPSMEFTd6.h:4739
NPSMEFTd6::Ceu_1122
double Ceu_1122
Definition: NPSMEFTd6.h:4717
NPSMEFTd6::muggH
virtual double muggH(const double sqrt_s) const
The ratio between the gluon-gluon fusion Higgs production cross-section in the current model and in ...
Definition: NPSMEFTd6.cpp:3623
gslpp::complex::i
static const complex & i()
Definition: gslpp_complex.cpp:154
NPSMEFTd6::eWH_1314_DHW
double eWH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4857
NPSMEFTd6::CLQ1_3323
double CLQ1_3323
Definition: NPSMEFTd6.h:4706
NPSMEFTd6::eVBF_78_HD
double eVBF_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4813
NPSMEFTd6::I_triangle_1
gslpp::complex I_triangle_1(const double tau, const double lambda) const
Loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3575
NPSMEFTd6::CdW_12i
double CdW_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4659
NPSMEFTd6::CQe_2322
double CQe_2322
Definition: NPSMEFTd6.h:4740
StandardModel::computeBrHtoZga
double computeBrHtoZga() const
The Br in the Standard Model.
Definition: StandardModel.h:2244
NPSMEFTd6::CLd_1133
double CLd_1133
Definition: NPSMEFTd6.h:4734
NPSMEFTd6::CeB_13r
double CeB_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4690
NPSMEFTd6::CuB_12r
double CuB_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4629
StandardModel::lambda
double lambda
The CKM parameter in the Wolfenstein parameterization.
Definition: StandardModel.h:2568
Particle::getCharge
double getCharge() const
A get method to access the particle charge.
Definition: Particle.h:97
NPSMEFTd6::deltaG3_hWW
virtual double deltaG3_hWW() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:3268
NPSMEFTd6::CeB_22i
double CeB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4697
NPSMEFTd6::CdW_12r
double CdW_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4653
NPSMEFTd6::deltaGL_f
double deltaGL_f(const Particle p) const
New physics contribution to the neutral-current left-handed coupling .
Definition: NPSMEFTd6.cpp:3176
NPSMEFTd6::deltaGammaTotalRatio1
virtual double deltaGammaTotalRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10909
StandardModel::computeBrHtogaga
double computeBrHtogaga() const
The Br in the Standard Model.
Definition: StandardModel.h:2256
NPSMEFTd6::CiHe_22
double CiHe_22
Definition: NPSMEFTd6.h:4943
StandardModel::computeSigmaggH
double computeSigmaggH(const double sqrt_s) const
The ggH cross section in the Standard Model.
Definition: StandardModel.h:1897
NPSMEFTd6::CdH_22i
double CdH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4601
NPSMEFTd6::CuH_33r
double CuH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4585
NPSMEFTd6::CHL3_23i
double CHL3_23i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4510
NPSMEFTd6::CHu_12r
double CHu_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4539
NPSMEFTd6::eWHmumu
double eWHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4786
NPSMEFTd6::eVBF_78_HG
double eVBF_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4817
NPSMEFTd6::eVBF_1314_HWB
double eVBF_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4830
NPSMEFTd6::CHe_13r
double CHe_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4513
NPSMEFTd6::eZH_1314_Hbox
double eZH_1314_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4886
NPSMEFTd6::aipHL
double aipHL
Definition: NPSMEFTd6.h:5038
NPSMEFTd6::eVBFHtautau
double eVBFHtautau
Definition: NPSMEFTd6.h:4785
NPSMEFTd6::lambdaH_tree
double lambdaH_tree
The SM tree level value of the scalar quartic coupling in the potential.
Definition: NPSMEFTd6.h:5020
NPSMEFTd6::eVBFint
double eVBFint
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4749
NPSMEFTd6::eZH_1314_HQ3_11
double eZH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4890
NPSMEFTd6::UevL
double UevL
The tree level value of the couplings in the SM. (Neglecting PMNS effects.)
Definition: NPSMEFTd6.h:5012
NPSMEFTd6::cLH3d62
double cLH3d62
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:5028
NPSMEFTd6::ettHpar
double ettHpar
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4748
NPSMEFTd6::CdG_11i
double CdG_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4646
NPSMEFTd6::eVBF_2_HQ3_11
double eVBF_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4798
NPSMEFTd6::CdW_11i
double CdW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4658
NPSMEFTd6::CeW_13i
double CeW_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4684
NPSMEFTd6::eZH_2_HQ1_11
double eZH_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4861
NPSMEFTd6::CHQ1_11
double CHQ1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4520
NPSMEFTd6::CuH_11i
double CuH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4586
NPSMEFTd6::Cee_1122
double Cee_1122
Definition: NPSMEFTd6.h:4714
NPSMEFTd6::eZH_1314_DeltaGF
double eZH_1314_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4897
StandardModel::computeSigmattH
double computeSigmattH(const double sqrt_s) const
The ttH production cross section in the Standard Model.
Definition: StandardModel.h:2171
NPSMEFTd6::CeH_33i
double CeH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4579
NPSMEFTd6::CuW_11r
double CuW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4616
NPSMEFTd6::eZHZga
double eZHZga
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::deltaGammaHbbRatio1
double deltaGammaHbbRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12663
NPSMEFTd6::CiDHW
double CiDHW
Definition: NPSMEFTd6.h:4959
NPSMEFTd6::AHZga_f
gslpp::complex AHZga_f(const double tau, const double lambda) const
Fermionic loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3605
NPSMEFTd6::CuH_12i
double CuH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4587
NPSMEFTd6::CdB_22r
double CdB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4667
NPSMEFTd6::CiuG_11r
double CiuG_11r
Definition: NPSMEFTd6.h:4978
NPSMEFTd6::CdH_12i
double CdH_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4599
NPSMEFTd6::CQe_2211
double CQe_2211
Definition: NPSMEFTd6.h:4738
NPSMEFTd6::CLQ3_1111
double CLQ3_1111
Definition: NPSMEFTd6.h:4708
NPSMEFTd6::obliqueW
virtual double obliqueW() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2942
NPSMEFTd6::deltaMz
virtual double deltaMz() const
The relative correction to the mass of the boson, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2954
NPSMEFTd6::CdG_33r
double CdG_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4645
NPSMEFTd6::deltaGwd6
virtual double deltaGwd6() const
The relative NP corrections to the width of the boson, .
Definition: NPSMEFTd6.cpp:3142
NPSMEFTd6::delta_AA
double delta_AA
Combination of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:5016
NPSMEFTd6::Cee_1111
double Cee_1111
Definition: NPSMEFTd6.h:4713
NPSMEFTd6::deltaGammaHgagaRatio2
double deltaGammaHgagaRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12467
NPSMEFTd6::CHd_23i
double CHd_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4555
NPSMEFTd6::CLQ3_1122
double CLQ3_1122
Definition: NPSMEFTd6.h:4709
NPSMEFTd6::eZH_2_Hbox
double eZH_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4860
NPSMEFTd6::CiuG_33r
double CiuG_33r
Definition: NPSMEFTd6.h:4980
NPSMEFTd6::CHQ1_23r
double CHQ1_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4524
NPSMEFTd6::CdG_33i
double CdG_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4651
NPSMEFTd6::CLQ3_2223
double CLQ3_2223
Definition: NPSMEFTd6.h:4711
NPSMEFTd6::CHQ3_13r
double CHQ3_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4531
NPSMEFTd6::CdW_33i
double CdW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4663
NPSMEFTd6::CHL1_22
double CHL1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4496
NPSMEFTd6::CHL3_12r
double CHL3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4503
NPSMEFTd6::CeW_22r
double CeW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4679
NPSMEFTd6::deltamb
virtual double deltamb() const
The relative correction to the mass of the quark, , with respect to ref. point used in the SM calcul...
Definition: NPSMEFTd6.cpp:2987
NPSMEFTd6::CHe_12r
double CHe_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4512
NPSMEFTd6::eWHZga
double eWHZga
Definition: NPSMEFTd6.h:4786
NPSMEFTd6::CHud_13i
double CHud_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4564
NPSMEFTd6::CuH_33i
double CuH_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4591
NPSMEFTd6::eZH_78_HW
double eZH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4880
NPSMEFTd6::CiHQ3_22
double CiHQ3_22
Definition: NPSMEFTd6.h:4939
NPSMEFTd6::CieH_33r
double CieH_33r
Definition: NPSMEFTd6.h:4968
NPSMEFTd6::CG
double CG
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4473
NPSMEFTd6::CuB_12i
double CuB_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4635
NPSMEFTd6::cLHd6
double cLHd6
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 inter...
Definition: NPSMEFTd6.h:5026
NPSMEFTd6::DeltaGF
virtual double DeltaGF() const
New physics contribution to the Fermi constant.
Definition: NPSMEFTd6.cpp:2922
NPSMEFTd6::CuB_13i
double CuB_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4636
NPSMEFTd6::CLQ3_3323
double CLQ3_3323
Definition: NPSMEFTd6.h:4711
NPSMEFTd6::eVBF_2_DHB
double eVBF_2_DHB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4804
StandardModel::GammaW
virtual double GammaW(const Particle fi, const Particle fj) const
A partial decay width of the boson decay into a SM fermion pair.
Definition: StandardModel.cpp:1166
cggHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:3034
NPSMEFTd6::BrHWW4fRatio
virtual double BrHWW4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10361
NPSMEFTd6::delta_h
double delta_h
Combinations of dimension 6 coefficients modifying the canonical field definition.
Definition: NPSMEFTd6.h:5018
NPSMEFTd6::CHbox
double CHbox
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4491
NPSMEFTd6::CdW_22r
double CdW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4655
NPSMEFTd6::CHF1_diag
double CHF1_diag(const Particle F) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle F.
Definition: NPSMEFTd6.cpp:2738
NPSMEFTd6::deltaG_hgg
virtual double deltaG_hgg() const
The new physics contribution to the coupling of the effective interaction .
Definition: NPSMEFTd6.cpp:3231
NPSMEFTd6::deltaGL_Wff
virtual gslpp::complex deltaGL_Wff(const Particle pbar, const Particle p) const
New physics contribution to the charged current coupling .
Definition: NPSMEFTd6.cpp:3207
NPSMEFTd6::CuB_11r
double CuB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4628
NPSMEFTd6::eepZBFpar
double eepZBFpar
Parametric relative theoretical error in via ZBF. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4764
NPSMEFTd6::ettHZga
double ettHZga
Definition: NPSMEFTd6.h:4788
NPSMEFTd6::NNPSMEFTd6Vars_LFU_QFU
static const int NNPSMEFTd6Vars_LFU_QFU
The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.
Definition: NPSMEFTd6.h:909
NPSMEFTd6::CeH_22i
double CeH_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4577
NPSMEFTd6::CHWHB_gagaorth
double CHWHB_gagaorth
The combination of dimension-6 operator coefficients .
Definition: NPSMEFTd6.h:4483
NPSMEFTd6::CiHd_22
double CiHd_22
Definition: NPSMEFTd6.h:4951
NPSMEFTd6::deltaGammaHZllRatio1
double deltaGammaHZllRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11505
NPSMEFTd6::CeW_33i
double CeW_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4687
NPSMEFTd6::CdB_12r
double CdB_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4665
NPSMEFTd6::eZHWW
double eZHWW
Definition: NPSMEFTd6.h:4787
NPSMEFTd6::dg1Z
double dg1Z
Independent contribution to aTGC.
Definition: NPSMEFTd6.h:4917
NPSMEFTd6::eZH_78_Hd_11
double eZH_78_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4876
NPSMEFTd6::eZH_78_HWB
double eZH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4881
NPSMEFTd6::CiuW_22r
double CiuW_22r
Definition: NPSMEFTd6.h:4983
NPSMEFTd6::eWHgaga
double eWHgaga
Definition: NPSMEFTd6.h:4786
NPSMEFTd6::eVBF_2_DeltaGF
double eVBF_2_DeltaGF
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4806
NPSMEFTd6::CLL_1133
double CLL_1133
Definition: NPSMEFTd6.h:4702
NPSMEFTd6::eZH_1314_HQ1_11
double eZH_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4887
NPSMEFTd6::CHQ1_22
double CHQ1_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4523
NPSMEFTd6::eHgagaint
double eHgagaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4773
NPSMEFTd6::CeW_13r
double CeW_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4678
NPSMEFTd6::CuG_13i
double CuG_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4612
NPSMEFTd6::eHtautaupar
double eHtautaupar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4778
NPSMEFTd6::CHB
double CHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4481
NPSMEFTd6::NPSMEFTd6Vars
static const std::string NPSMEFTd6Vars[NNPSMEFTd6Vars]
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotat...
Definition: NPSMEFTd6.h:897
NPSMEFTd6::deltaytau_HB
virtual double deltaytau_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15491
NPSMEFTd6::eVBF_1314_Hu_11
double eVBF_1314_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4824
NPSMEFTd6::CiHd_11
double CiHd_11
Definition: NPSMEFTd6.h:4950
NPSMEFTd6::CLL_2211
double CLL_2211
Definition: NPSMEFTd6.h:4701
NPSMEFTd6::eZH_78_DHW
double eZH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4883
NPSMEFTd6::eZH_78_DHB
double eZH_78_DHB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4882
NPSMEFTd6::gZuL
double gZuL
Definition: NPSMEFTd6.h:5009
NPSMEFTd6::deltaGammaHWWRatio2
double deltaGammaHWWRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11069
NPSMEFTd6::sW2_tree
double sW2_tree
The square of the tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:5001
NPSMEFTd6::STXS_qqHqq_Rest
virtual double STXS_qqHqq_Rest(const double sqrt_s) const
The STXS bin .
Definition: NPSMEFTd6.cpp:15188
NPSMEFTd6::eVBF_2_Hbox
double eVBF_2_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4794
NPSMEFTd6::CH
double CH
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4492
NPSMEFTd6::Ced_3323
double Ced_3323
Definition: NPSMEFTd6.h:4723
NPSMEFTd6::CLd_1123
double CLd_1123
Definition: NPSMEFTd6.h:4735
NPSMEFTd6::ettHtautau
double ettHtautau
Definition: NPSMEFTd6.h:4788
NPSMEFTd6::CHQ3_12r
double CHQ3_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4530
NPSMEFTd6::Yuktau
double Yuktau
SM lepton Yukawas.
Definition: NPSMEFTd6.h:5030
NPSMEFTd6::lambdaZNP
virtual double lambdaZNP() const
The new physics contribution to the anomalous triple gauge coupling .
Definition: NPSMEFTd6.cpp:13850
NPSMEFTd6::muVBF
virtual double muVBF(const double sqrt_s) const
The ratio between the vector-boson fusion Higgs production cross-section in the current model and in...
Definition: NPSMEFTd6.cpp:3758
NPSMEFTd6::CHQ3_11
double CHQ3_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4529
NPSMEFTd6::CLu_1133
double CLu_1133
Definition: NPSMEFTd6.h:4730
NPSMEFTd6::eVBFHmumu
double eVBFHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4785
StandardModel::computeSigmaZH
double computeSigmaZH(const double sqrt_s) const
The ZH production cross section in the Standard Model.
Definition: StandardModel.h:2135
NPSMEFTd6::eVBF_2_Hd_11
double eVBF_2_Hd_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4797
NPSMEFTd6::CiHQ1_11
double CiHQ1_11
Definition: NPSMEFTd6.h:4935
NPSMEFTd6::Ced_1132
double Ced_1132
Definition: NPSMEFTd6.h:4724
NPSMEFTd6::CfH_diag
gslpp::complex CfH_diag(const Particle f) const
The diagonal entry of the dimension-6 operator coefficient corresponding to particle f.
Definition: NPSMEFTd6.cpp:2815
NPSMEFTd6::eeeWBFpar
double eeeWBFpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4756
NPSMEFTd6::CeW_23i
double CeW_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4686
NPSMEFTd6::deltaGamma_Wff
virtual double deltaGamma_Wff(const Particle fi, const Particle fj) const
The new physics contribution to the decay width of the boson into a given fermion pair,...
Definition: NPSMEFTd6.cpp:3090
NPSMEFTd6::CDHB
double CDHB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4484
NPSMEFTd6::CdH_11r
double CdH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4592
NPSMEFTd6::cZga_HB
virtual double cZga_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15558
StandardModel::computeBrHtocc
double computeBrHtocc() const
The Br in the Standard Model.
Definition: StandardModel.h:2290
NPSMEFTd6::aiHW
double aiHW
Definition: NPSMEFTd6.h:5036
NPSMEFTd6::eHWWint
double eHWWint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4767
NPSMEFTd6::eZH_2_DHW
double eZH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4870
NPSMEFTd6::deltaGammaHZZ4vRatio1
double deltaGammaHZZ4vRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12002
NPSMEFTd6::CdB_13i
double CdB_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4672
NPSMEFTd6::CdH_11i
double CdH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4598
NPSMEFTd6::CuB_33i
double CuB_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4639
NPSMEFTd6::eZH_78_HB
double eZH_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4879
NPSMEFTd6::eZH_1314_DHW
double eZH_1314_DHW
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4896
NPSMEFTd6::deltaGammaHZllRatio2
double deltaGammaHZllRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11538
NPSMEFTd6::FlagRotateCHWCHB
bool FlagRotateCHWCHB
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and ...
Definition: NPSMEFTd6.h:5105
NPSMEFTd6::CHd_22
double CHd_22
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4550
NPSMEFTd6::eZH_2_HB
double eZH_2_HB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4866
NPSMEFTd6::CdB_11r
double CdB_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4664
NPSMEFTd6::CLQ3_2112
double CLQ3_2112
Definition: NPSMEFTd6.h:4709
NPSMEFTd6::eWH_78_Hbox
double eWH_78_Hbox
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4844
NPSMEFTd6::deltaGammaHggRatio1
double deltaGammaHggRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10988
StandardModel::Mw_tree
virtual double Mw_tree() const
The tree-level mass of the boson, .
Definition: StandardModel.cpp:951
NPSMEFTd6::BrHZuuRatio
virtual double BrHZuuRatio() const
The ratio of the Br ( ) in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10566
NPSMEFTd6::mueeZHPol
virtual double mueeZHPol(const double sqrt_s, const double Pol_em, const double Pol_ep) const
The ratio between the associated production cross-section in the current model and in the Standard ...
Definition: NPSMEFTd6.cpp:7910
NPSMEFTd6::BrHZZ4vRatio
virtual double BrHZZ4vRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10541
NPSMEFTd6::CuG_11r
double CuG_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4604
NPSMEFTd6::eWH_78_HD
double eWH_78_HD
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4846
NPSMEFTd6::eWHpar
double eWHpar
Parametric relative theoretical error in WH production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4752
NPSMEFTd6::eHZZpar
double eHZZpar
Parametric relative theoretical error in .
Definition: NPSMEFTd6.h:4770
NPSMEFTd6::eVBF_78_HQ1_11
double eVBF_78_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4809
StandardModel::computeBrHtomumu
double computeBrHtomumu() const
The Br in the Standard Model.
Definition: StandardModel.h:2267
NPSMEFTd6::eVBF_1314_HW
double eVBF_1314_HW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4829
StandardModel::computeSigmaVBF
double computeSigmaVBF(const double sqrt_s) const
The VBF cross section in the Standard Model.
Definition: StandardModel.h:2003
NPSMEFTd6::deltaGammaHWWRatio1
double deltaGammaHWWRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11049
NPSMEFTd6::eVBF_1314_HQ1_11
double eVBF_1314_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4823
NPSMEFTd6::deltaGammaHZffRatio2
double deltaGammaHZffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:12220
NPSMEFTd6::aiHd
double aiHd
Definition: NPSMEFTd6.h:5038
NPSMEFTd6::CuH_23r
double CuH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4584
NPSMEFTd6::CDB
double CDB
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4486
NPSMEFTd6::CeB_22r
double CeB_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4691
StandardModel::computeBrHtoWW
double computeBrHtoWW() const
The Br in the Standard Model.
Definition: StandardModel.h:2210
NPSMEFTd6::eeettHint
double eeettHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4759
NPSMEFTd6::eWH_78_HW
double eWH_78_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4847
NPSMEFTd6::CHud_12r
double CHud_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4557
NPSMEFTd6::Yukb
double Yukb
SM d-quark Yukawas.
Definition: NPSMEFTd6.h:5032
NPSMEFTd6::eggFpar
double eggFpar
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4746
NPSMEFTd6::CdG_22i
double CdG_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4649
NPSMEFTd6::CdB_22i
double CdB_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4673
NPSMEFTd6::CiHQ1_33
double CiHQ1_33
Definition: NPSMEFTd6.h:4937
NPSMEFTd6::aiHu
double aiHu
Definition: NPSMEFTd6.h:5038
NPSMEFTd6::deltaGammaHZZ2e2muRatio1
double deltaGammaHZZ2e2muRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11819
QCD::STRANGE
Definition: QCD.h:327
NPSMEFTd6::ettH_78_HG
double ettH_78_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4904
NPSMEFTd6::deltaaSMZ
virtual double deltaaSMZ() const
The relative correction to the strong coupling constant at the Z pole, , with respect to ref....
Definition: NPSMEFTd6.cpp:3053
NPSMEFTd6::CuW_23r
double CuW_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4620
NPSMEFTd6::deltaGammaHZvvRatio2
double deltaGammaHZvvRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11976
NPSMEFTd6::deltaGammaHZZ4fRatio2
double deltaGammaHZZ4fRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:12306
NPSMEFTd6::eVBF_2_Hu_11
double eVBF_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4796
NPSMEFTd6::eVBF_78_Hu_11
double eVBF_78_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4810
NPSMEFTd6::BrHZgaRatio
virtual double BrHZgaRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10699
NPSMEFTd6::eWH_2_DHW
double eWH_2_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (1...
Definition: NPSMEFTd6.h:4841
NPSMEFTd6::Cee_3311
double Cee_3311
Definition: NPSMEFTd6.h:4715
NPSMEFTd6::CiHu_33
double CiHu_33
Definition: NPSMEFTd6.h:4948
NPSMEFTd6::CLQ1_1111
double CLQ1_1111
Definition: NPSMEFTd6.h:4703
gslpp::complex::real
const double & real() const
Definition: gslpp_complex.cpp:53
NPSMEFTd6::Yuke
double Yuke
Definition: NPSMEFTd6.h:5030
NPSMEFTd6::CiHQ3_33
double CiHQ3_33
Definition: NPSMEFTd6.h:4940
NPSMEFTd6::CHud_23r
double CHud_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4560
NPSMEFTd6::deltaGammaHccRatio2
double deltaGammaHccRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12638
NPSMEFTd6::ettHmumu
double ettHmumu
Total relative theoretical error in .
Definition: NPSMEFTd6.h:4788
NPSMEFTd6::Ced_1111
double Ced_1111
Definition: NPSMEFTd6.h:4720
NPSMEFTd6::CdB_23r
double CdB_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4668
StandardModel::leptons
Particle leptons[6]
An array of Particle objects for the leptons.
Definition: StandardModel.h:2540
NPSMEFTd6::g2_tree
double g2_tree
The tree level value of the gauge coupling contant (at the pole).
Definition: NPSMEFTd6.h:5004
NPSMEFTd6::aiB
double aiB
Definition: NPSMEFTd6.h:5036
NPSMEFTd6::deltaGammaHWlvRatio1
double deltaGammaHWlvRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11097
NPSMEFTd6::deltaGammaHZZRatio2
double deltaGammaHZZRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11477
NPSMEFTd6::muttH
virtual double muttH(const double sqrt_s) const
The ratio between the t-tbar-Higgs associated production cross-section in the current model and in t...
Definition: NPSMEFTd6.cpp:9078
NPSMEFTd6::CiLL_1221
double CiLL_1221
Definition: NPSMEFTd6.h:4990
NPSMEFTd6::dGammaHTotR2
double dGammaHTotR2
Definition: NPSMEFTd6.h:5042
StandardModel::GammaZ
virtual double GammaZ(const Particle f) const
The partial decay width, .
Definition: StandardModel.cpp:1227
Particle::getIndex
int getIndex() const
Definition: Particle.h:160
NPSMEFTd6::CdG_13i
double CdG_13i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4648
NPSMEFTd6::CLQ3_1123
double CLQ3_1123
Definition: NPSMEFTd6.h:4711
NPSMEFTd6::BrHZgamumuRatio
virtual double BrHZgamumuRatio() const
The ratio of the Br in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10751
NPSMEFTd6::Cee_1133
double Cee_1133
Definition: NPSMEFTd6.h:4715
NPSMEFTd6::CuW_23i
double CuW_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4626
NPSMEFTd6::Ced_2232
double Ced_2232
Definition: NPSMEFTd6.h:4724
NPSMEFTd6::eVBFHZga
double eVBFHZga
Definition: NPSMEFTd6.h:4785
NPSMEFTd6::C2WS
double C2WS
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4478
NPSMEFTd6::CeW_11i
double CeW_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4682
NPSMEFTd6::CLL_1331
double CLL_1331
Definition: NPSMEFTd6.h:4702
NPSMEFTd6::GammaHZZRatio
double GammaHZZRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:11441
NPSMEFTd6::deltaGammaHtautauRatio2
double deltaGammaHtautauRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12572
NPSMEFTd6::CHd_12i
double CHd_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4553
NPSMEFTd6::FlagUnivOfX
bool FlagUnivOfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and ...
Definition: NPSMEFTd6.h:5108
NPbase::PostUpdate
virtual bool PostUpdate()
The postupdate method for NPbase.
Definition: NPbase.cpp:23
StandardModel::computeBrHtogg
double computeBrHtogg() const
The Br in the Standard Model.
Definition: StandardModel.h:2199
NPSMEFTd6::CiHWB
double CiHWB
Definition: NPSMEFTd6.h:4960
NPSMEFTd6::Ced_1133
double Ced_1133
Definition: NPSMEFTd6.h:4722
Model::name
std::string name
The name of the model.
Definition: Model.h:275
NPSMEFTd6::aiH
double aiH
Definition: NPSMEFTd6.h:5036
NPSMEFTd6::aiHe
double aiHe
Definition: NPSMEFTd6.h:5038
StandardModel::Mz
double Mz
The mass of the boson in GeV.
Definition: StandardModel.h:2554
Model::setModelLinearized
void setModelLinearized(bool linearized=true)
Definition: Model.h:231
NPSMEFTd6::CLQ1_2112
double CLQ1_2112
Definition: NPSMEFTd6.h:4704
NPSMEFTd6::CiuH_22r
double CiuH_22r
Definition: NPSMEFTd6.h:4971
NPSMEFTd6::deltaGV_f
virtual double deltaGV_f(const Particle p) const
New physics contribution to the neutral-current vector coupling .
Definition: NPSMEFTd6.cpp:3166
NPSMEFTd6::deltaGammaHWffRatio2
double deltaGammaHWffRatio2() const
The new physics contribution to the ratio of the , with any fermion, in the current model and in the...
Definition: NPSMEFTd6.cpp:11361
NPSMEFTd6::ettH_2_HG
double ettH_2_HG
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4899
NPSMEFTd6::CiHL1_11
double CiHL1_11
Definition: NPSMEFTd6.h:4928
NPSMEFTd6::eeeZHpar
double eeeZHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4758
NPSMEFTd6::CLL_2112
double CLL_2112
Definition: NPSMEFTd6.h:4701
QCD::Nc
double Nc
The number of colours.
Definition: QCD.h:932
NPSMEFTd6::CiDHB
double CiDHB
Definition: NPSMEFTd6.h:4958
NPSMEFTd6::CiW
double CiW
Definition: NPSMEFTd6.h:4954
NPSMEFTd6::CHL1_11
double CHL1_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4493
StandardModel::computeBrHtoZZinv
double computeBrHtoZZinv() const
The Br in the Standard Model.
Definition: StandardModel.h:2233
NPSMEFTd6::AHZga_W
gslpp::complex AHZga_W(const double tau, const double lambda) const
W loop function entering in the calculation of the effective coupling.
Definition: NPSMEFTd6.cpp:3610
NPSMEFTd6::BrHZZ4fRatio
virtual double BrHZZ4fRatio() const
The ratio of the Br , with any fermion, in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10674
NPSMEFTd6::CuB_11i
double CuB_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4634
NPSMEFTd6::dxseeWWdcos
virtual double dxseeWWdcos(const double sqrt_s, const double cos) const
The differential distribution for , with , as a function of the polar angle.
Definition: NPSMEFTd6.cpp:13889
NPSMEFTd6::eVBFpar
double eVBFpar
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy....
Definition: NPSMEFTd6.h:4750
NPSMEFTd6::CeH_11i
double CeH_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4574
NPSMEFTd6::CuG_33i
double CuG_33i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4615
NPSMEFTd6::CeW_11r
double CeW_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4676
NPSMEFTd6::eeettHpar
double eeettHpar
Parametric relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4760
lambdaZ
An observable class for the anomalous triple gauge coupling .
Definition: aTGC.h:99
NPSMEFTd6::f_triangle
gslpp::complex f_triangle(const double tau) const
Loop function entering in the calculation of the effective and couplings.
Definition: NPSMEFTd6.cpp:3551
NPSMEFTd6::CLQ3_1221
double CLQ3_1221
Definition: NPSMEFTd6.h:4709
NPSMEFTd6::CdH_23i
double CdH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4602
StandardModel::Mw
virtual double Mw() const
The SM prediction for the -boson mass in the on-shell scheme, .
Definition: StandardModel.cpp:970
NPSMEFTd6::CDW
double CDW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4487
NPSMEFTd6::eZH_2_HWB
double eZH_2_HWB
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4868
NPSMEFTd6::eWH_2_HQ3_11
double eWH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4837
NPSMEFTd6::eVBF_2_HQ1_11
double eVBF_2_HQ1_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4795
convertToGslFunction
gsl_function convertToGslFunction(const F &f)
Definition: gslpp_function_adapter.h:24
NPSMEFTd6::deltaGR_f
double deltaGR_f(const Particle p) const
New physics contribution to the neutral-current right-handed coupling .
Definition: NPSMEFTd6.cpp:3191
NPSMEFTd6::Ced_1123
double Ced_1123
Definition: NPSMEFTd6.h:4723
NPSMEFTd6::Ceu_2233
double Ceu_2233
Definition: NPSMEFTd6.h:4719
NPSMEFTd6::deltaGammaHWjjRatio1
double deltaGammaHWjjRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11214
NPSMEFTd6::CeH_23i
double CeH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4578
NPSMEFTd6::deltaGammaHZZ2e2muRatio2
double deltaGammaHZZ2e2muRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11856
NPSMEFTd6::CuG_22r
double CuG_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4607
NPSMEFTd6::muWH
virtual double muWH(const double sqrt_s) const
The ratio between the W-Higgs associated production cross-section in the current model and in the St...
Definition: NPSMEFTd6.cpp:7188
NPSMEFTd6::deltaGammaHmumuRatio2
double deltaGammaHmumuRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12519
NPSMEFTd6::CHu_23r
double CHu_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4542
NPSMEFTd6::eVBF_78_HQ3_11
double eVBF_78_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4812
NPSMEFTd6::deltayt_HB
virtual double deltayt_HB() const
The Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition ...
Definition: NPSMEFTd6.cpp:15469
NPSMEFTd6::CiHL3_11
double CiHL3_11
Definition: NPSMEFTd6.h:4931
NPSMEFTd6::CLL_3113
double CLL_3113
Definition: NPSMEFTd6.h:4702
NPSMEFTd6::ettH_2_G
double ettH_2_G
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at Tevatron ...
Definition: NPSMEFTd6.h:4900
NPSMEFTd6::CeH_12r
double CeH_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4569
NPSMEFTd6::Yuks
double Yuks
Definition: NPSMEFTd6.h:5032
NPSMEFTd6::gZdR
double gZdR
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:5010
NPSMEFTd6::CLQ1_3311
double CLQ1_3311
Definition: NPSMEFTd6.h:4705
NPSMEFTd6::eeeZHint
double eeeZHint
Intrinsic relative theoretical error in . (Assumed to be constant in energy.)
Definition: NPSMEFTd6.h:4757
NPSMEFTd6::CHe_12i
double CHe_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4517
NPSMEFTd6::C2B
double C2B
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4475
NPSMEFTd6::deltaGammaHtautauRatio1
double deltaGammaHtautauRatio1() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12545
NPSMEFTd6::eWH_78_HWB
double eWH_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4848
NPSMEFTd6::CHD
double CHD
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4489
NPSMEFTd6::CLe_3311
double CLe_3311
Definition: NPSMEFTd6.h:4727
NPSMEFTd6::eHbbint
double eHbbint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4781
NPSMEFTd6::eVBF_2_HD
double eVBF_2_HD
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4799
NPSMEFTd6::CuB_23i
double CuB_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4638
NPSMEFTd6::CHQ3_33
double CHQ3_33
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4534
NPSMEFTd6::eZH_2_HQ3_11
double eZH_2_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4864
NPSMEFTd6::deltaGammaHWW4jRatio2
double deltaGammaHWW4jRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11304
NPSMEFTd6::deltaGammaHZddRatio1
double deltaGammaHZddRatio1() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:12124
NPSMEFTd6::sW_tree
double sW_tree
The tree level values for the sine of the weak angle.
Definition: NPSMEFTd6.h:4999
NPSMEFTd6::eVBFHZZ
double eVBFHZZ
Definition: NPSMEFTd6.h:4785
NPSMEFTd6::deltaGammaTotalRatio2
virtual double deltaGammaTotalRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:10953
NPSMEFTd6::CdH_33r
double CdH_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4597
NPSMEFTd6::eHZgaint
double eHZgaint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4771
NPSMEFTd6::CdB_23i
double CdB_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4674
NPSMEFTd6::eHZZint
double eHZZint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4769
StandardModel::Gamma_Z
virtual double Gamma_Z() const
The total decay width of the boson, .
Definition: StandardModel.cpp:1344
NPSMEFTd6::CHQ1_12i
double CHQ1_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4526
NPSMEFTd6::deltaGamma_W
virtual double deltaGamma_W() const
The new physics contribution to the total decay width of the boson, .
Definition: NPSMEFTd6.cpp:3124
NPSMEFTd6::eWH_2_HW
double eWH_2_HW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4839
NPSMEFTd6::NPSMEFTd6M
Matching< NPSMEFTd6Matching, NPSMEFTd6 > NPSMEFTd6M
Definition: NPSMEFTd6.h:4471
NPSMEFTd6::eZH_2_Hu_11
double eZH_2_Hu_11
Theoretical uncertainty in the (linear) new physics contribution from to ZH production at Tevatron (...
Definition: NPSMEFTd6.h:4862
QCD::DOWN
Definition: QCD.h:325
cZgaHB
An observable class for the Higgs-basis coupling . (See LHCHXSWG-INT-2015-001 document....
Definition: NP_couplings.h:2958
NPSMEFTd6::eVBF_78_DHW
double eVBF_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4819
NPSMEFTd6::CHud_22r
double CHud_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4559
NPSMEFTd6::CuW_22r
double CuW_22r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4619
NPSMEFTd6::eWH_1314_HWB
double eWH_1314_HWB
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4856
NPSMEFTd6::eVBFHWW
double eVBFHWW
Definition: NPSMEFTd6.h:4785
NPSMEFTd6::deltaGammaHZZ4eRatio2
double deltaGammaHZZ4eRatio2() const
The new physics contribution to the ratio of the in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11793
NPSMEFTd6::CiHbox
double CiHbox
Definition: NPSMEFTd6.h:4962
NPSMEFTd6::CHQ1_12r
double CHQ1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4521
NPSMEFTd6::ettH_1314_uG_33r
double ettH_1314_uG_33r
Theoretical uncertainty in the (linear) new physics contribution from to ttH production at the LHC (...
Definition: NPSMEFTd6.h:4911
NPSMEFTd6::eWH_78_DHW
double eWH_78_DHW
Theoretical uncertainty in the (linear) new physics contribution from to WH production at the LHC (7...
Definition: NPSMEFTd6.h:4849
NPSMEFTd6::CT
double CT
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4490
NPSMEFTd6::CuW_12r
double CuW_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4617
NPSMEFTd6::dGammaHTotR1
double dGammaHTotR1
Definition: NPSMEFTd6.h:5042
NPSMEFTd6::CuW_22i
double CuW_22i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4625
NPSMEFTd6::eVBF_78_HB
double eVBF_78_HB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4814
NPSMEFTd6::CdB_33r
double CdB_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4669
NPSMEFTd6::GammaHggRatio
double GammaHggRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:10972
NPSMEFTd6::CHQ1_13r
double CHQ1_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4522
NPSMEFTd6::CiHL3_33
double CiHL3_33
Definition: NPSMEFTd6.h:4933
NPSMEFTd6::CLQ3_2232
double CLQ3_2232
Definition: NPSMEFTd6.h:4712
NPSMEFTd6::CHe_11
double CHe_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4511
NPSMEFTd6::obliqueY
virtual double obliqueY() const
The oblique parameter . (Simplified implementation. Contribution only from .)
Definition: NPSMEFTd6.cpp:2947
NPSMEFTd6::CdB_13r
double CdB_13r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4666
NPSMEFTd6::GammaHbbRatio
double GammaHbbRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12648
NPSMEFTd6::eHmumuint
double eHmumuint
Intrinsic relative theoretical error in .
Definition: NPSMEFTd6.h:4775
NPSMEFTd6::eHwidth
double eHwidth
Total relative theoretical error in the Higgs width.
Definition: NPSMEFTd6.h:4791
NPSMEFTd6::deltaGammaHZZ4lRatio2
double deltaGammaHZZ4lRatio2() const
The new physics contribution to the ratio of the ( ) in the current model and in the Standard Model....
Definition: NPSMEFTd6.cpp:11730
QCD::NEUTRINO_1
Definition: QCD.h:311
NPSMEFTd6::ettHZZ
double ettHZZ
Definition: NPSMEFTd6.h:4788
QCD::quarks
Particle quarks[6]
The vector of all SM quarks.
Definition: QCD.h:934
NPSMEFTd6::CHu_11
double CHu_11
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4538
NPSMEFTd6::CLQ1_1133
double CLQ1_1133
Definition: NPSMEFTd6.h:4705
NPSMEFTd6::CHud_11i
double CHud_11i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4562
NPSMEFTd6::CW
double CW
The dimension-6 operator coefficient .
Definition: NPSMEFTd6.h:4474
NPSMEFTd6::aiu
double aiu
Definition: NPSMEFTd6.h:5039
NPSMEFTd6::eVBF_78_HWB
double eVBF_78_HWB
Theoretical uncertainty in the (linear) new physics contribution from to VBF production at Tevatron ...
Definition: NPSMEFTd6.h:4816
NPSMEFTd6::CuH_11r
double CuH_11r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4580
NPSMEFTd6::gZvL
double gZvL
The tree level value of the couplings in the SM.
Definition: NPSMEFTd6.h:5007
QCD::MU
Definition: QCD.h:314
NPSMEFTd6::CHL3_23r
double CHL3_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4506
NPSMEFTd6::CuH_23i
double CuH_23i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4590
NPSMEFTd6::CiHe_11
double CiHe_11
Definition: NPSMEFTd6.h:4942
NPbase::deltaGamma_Zf
virtual double deltaGamma_Zf(const Particle f) const
The new physics contribution to the decay width of the boson into a given fermion pair,...
Definition: NPbase.cpp:135
NPSMEFTd6::CdB_12i
double CdB_12i
The dimension-6 operator coefficient (imaginary part).
Definition: NPSMEFTd6.h:4671
NPSMEFTd6::aiG
double aiG
Definition: NPSMEFTd6.h:5035
NPSMEFTd6::CeW_33r
double CeW_33r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4681
NPSMEFTd6::Br_H_inv
virtual double Br_H_inv() const
The branching ratio of the of the Higgs into invisible particles.
Definition: NPSMEFTd6.cpp:12720
NPSMEFTd6::CdH_23r
double CdH_23r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4596
NPSMEFTd6::Yukc
double Yukc
Definition: NPSMEFTd6.h:5031
NPSMEFTd6::GammaHgagaRatio
double GammaHgagaRatio() const
The ratio of the in the current model and in the Standard Model.
Definition: NPSMEFTd6.cpp:12401
NPSMEFTd6::CHL3_13i
double CHL3_13i
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4509
NPSMEFTd6::CLe_1122
double CLe_1122
Definition: NPSMEFTd6.h:4726
NPSMEFTd6::CHL1_12r
double CHL1_12r
The dimension-6 operator coefficient (real part).
Definition: NPSMEFTd6.h:4494
NPSMEFTd6::FlagFlavU3OfX
bool FlagFlavU3OfX
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.
Definition: NPSMEFTd6.h:5107
NPSMEFTd6::eWH_1314_HQ3_11
double eWH_1314_HQ3_11
Theoretical uncertainty in the (linear) new physics contribution from to WH production at Tevatron (...
Definition: NPSMEFTd6.h:4853